Optical path bending type zoom lens system and image taking apparatus including the same

ABSTRACT

A zoom lens system comprises, in order from an object side, a positive first lens unit including a reflective optical element, a negative second lens unit, a positive third lens unit and a positive fourth lens unit, or a positive first lens unit, a negative second lens unit, a positive third lens unit, a negative fourth lens unit and a positive fifth lens unit. During zooming from a wide-angle end toward a telephoto end, the first lens unit is fixed, at least the second and third lens units move, and a space between the lens units changes. The second lens unit is positioned closer to an image-surface side in the telephoto end than in the wide-angle end, and the third lens unit is positioned closer to the object side in the telephoto end than in the wide-angle end. An image taking apparatus including the zoom lens system is also disclosed.

CROSS REFERENCE TO RELATED APPLICATION

This application claims benefit under 35 U.S.C. §119 of Japanese PatentApplications of No. 2005-170503, filed in Japan on June 10 and No.2005-180641, filed in Japan on Jun. 21, 2005, the contents of which areincorporated herein by reference.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to an optical path bending type zoom lenssystem and an image taking apparatus including the same.

2. Description of the Related Art

Heretofore, an optical path bending type zoom lens has been known inwhich an optical path is bent to thereby reduce a thickness of the lenssystem as much as possible in an incidence optical axis direction. Insuch zoom lens system, a first lens unit is provided with a reflectivesurface, and a movable lens unit which moves during zooming is disposedin an optical path after reflection. Therefore, when this zoom lenssystem is incorporated into a camera, a moving direction of the lensunit which moves during the zooming is a height direction or a lateraldirection of the camera. Therefore, a zoom lens system having a highzooming ratio can be used while reducing a camera thickness (length in adirection from an object toward a photographer).

As such zoom lens system, there are known zoom lens systems described inJapanese Patent Application Laid-Open Nos. 2000-131,610, 2003-202,500,2003-302,576, 2003-329,932 and 2004-184,627.

SUMMARY OF THE INVENTION

The present invention provides a zoom lens system which includes areflective surface to bend an optical path and whose thickness in anincidence optical axis direction is reduced as much as possible, and animage taking apparatus including the same.

In the present invention, a first type of zoom lens system comprises, inorder from an object side: a first lens unit having a positiverefractive power; a second lens unit having a negative refractive power;a third lens unit having a positive refractive power; and a fourth lensunit having a positive refractive power,

the zoom lens system having four lens units in total,

during zooming from a wide-angle end toward a telephoto end, the firstlens unit being fixed, at least the second lens unit and the third lensunit being moved, and a space between the third lens unit and the fourthlens unit being changed,

the second lens unit being positioned closer to an image-surface side inthe telephoto end than in the wide-angle end,

the third lens unit being positioned closer to the object side in thetelephoto end than in the wide-angle end,

the first lens unit comprising a reflective optical element whichreflects an optical path,

the zoom lens system satisfying the following condition:

0.5<f _(1G) /f _(w)<3.5  (1A),

wherein f_(1G) denotes a focal length of the first lens unit, and f_(w)denotes a focal length of the zoom lens system in the wide-angle end.

In the present invention, a first type of image taking apparatuscomprises:

a zoom lens system; and

an image sensor which is disposed on an image side of the zoom lenssystem, which has a light receiving surface and which converts anoptical image formed by the zoom lens system into an electric signal,

the zoom lens system comprising, in order from an object side:

a first lens unit having a positive refractive power; a second lens unithaving a negative refractive power; a third lens unit having a positiverefractive power; and a fourth lens unit having a positive refractivepower,

the zoom lens system having four lens units in total,

during zooming from a wide-angle end toward a telephoto end, the firstlens unit being fixed to an image surface on the light receivingsurface, at least the second lens unit and the third lens unit beingmoved, and a space between the third lens unit and the fourth lens unitbeing changed,

the second lens unit being positioned closer to an image-surface side inthe telephoto end than in the wide-angle end,

the third lens unit being positioned closer to the object side in thetelephoto end than in the wide-angle end,

the first lens unit comprising a reflective optical element whichreflects an optical path,

the apparatus satisfying the following conditions:

1.6<f _(w) /ih<1.9  (6A); and

0.85<f _(1G) /ih<6.0  (7A),

wherein f_(1G) denotes a focal length of the first lens unit, f_(w)denotes a focal length of the zoom lens system in the wide-angle end,and ih denotes a maximum image height in an effective image takingregion of the light receiving surface.

In the present invention, a second type of image taking apparatuscomprises:

a zoom lens system; and

an image sensor which is disposed on an image side of the zoom lenssystem, which has a light receiving surface and which converts anoptical image formed by the zoom lens system into an electric signal,

the zoom lens system comprising, in order from an object side:

a first lens unit having a positive refractive power; a second lens unithaving a negative refractive power; a third lens unit having a positiverefractive power; and a fourth lens unit having a positive refractivepower,

the zoom lens system having four lens units in total,

during zooming from a wide-angle end toward a telephoto end, the firstlens unit being fixed, at least the second lens unit and the third lensunit being moved, and a space between the third lens unit and the fourthlens unit being changed,

the second lens unit being positioned closer to an image-surface side inthe telephoto end than in the wide-angle end,

the third lens unit being positioned closer to the object side in thetelephoto end than in the wide-angle end,

the first lens unit comprising a reflective optical element whichreflects an optical path,

the apparatus satisfying the following conditions:

1.6<f _(w) /ih<1.9  (6A);

0.85<|f _(2G) /ih|<3.1  (8A);

1.0<f _(3G) /ih<3.7  (15A); and

0.7<m _(2GZ)/m_(3GZ)<1.2  (3A),

wherein f_(w) denotes a focal length of the zoom lens system in thewide-angle end, f_(2G) denotes a focal length of the second lens unit,f_(3G) denotes a focal length of the third lens unit, ih denotes amaximum image height in an effective image taking region of the lightreceiving surface, m_(2GZ) denotes a ratio of a magnification of thesecond lens unit in the telephoto end to that in the wide-angle end whenthe zoom lens system if focused on an infinite object, and m_(3GZ)denotes a ratio of a magnification of the third lens unit in thetelephoto end to that in the wide-angle end when the zoom lens system isfocused on the infinite object.

In the present invention, a second type of zoom lens system comprises,in order from an object side:

a first lens unit having a positive refractive power; a second lens unithaving a negative refractive power; a third lens unit having a positiverefractive power; a fourth lens unit having a negative refractive power;and a fifth lens unit having a positive refractive power,

the zoom lens system having five lens units in total,

during zooming from a wide-angle end toward a telephoto end, the firstlens unit being fixed, at least the second lens unit and the third lensunit being moved, and a space between the lens units being changed,

the second lens unit being positioned closer to an image-surface side inthe telephoto end than in the wide-angle end,

the third lens unit being positioned closer to the object side in thetelephoto end than in the wide-angle end,

the first lens unit comprising a reflective optical element whichreflects an optical path,

the zoom lens system satisfying the following condition:

0.5<f _(1G) /f _(w)<3.5  (1B),

wherein f_(1G) denotes a focal length of the first lens unit, and f_(w)denotes a focal length of the zoom lens system in the wide-angle end.

In the present invention, a third type of image taking apparatuscomprises:

a zoom lens system; and

an image sensor which is disposed on an image side of the zoom lenssystem, which has a light receiving surface and which converts anoptical image formed by the zoom lens system into an electric signal,

the zoom lens system comprising, in order from an object side:

a first lens unit having a positive refractive power; a second lens unithaving a negative refractive power; a third lens unit having a positiverefractive power; a fourth lens unit having a negative refractive power;and a fifth lens unit having a positive refractive power,

the zoom lens system having five lens units in total,

during zooming from a wide-angle end toward a telephoto end, the firstlens unit being fixed to an image surface on the light receivingsurface, at least the second lens unit and the third lens unit beingmoved, and a space between the lens units being changed,

the second lens unit being positioned closer to an image-surface side inthe telephoto end than in the wide-angle end,

the third lens unit being positioned closer to the object side in thetelephoto end than in the wide-angle end,

the first lens unit comprising a reflective optical element whichreflects an optical path,

the apparatus satisfying the following conditions:

1.5<f _(w) /ih<1.9  (6B); and

0.85<f _(1G) /ih<6.0  (7B),

wherein f_(1G) denotes a focal length of the first lens unit, f_(w)denotes a focal length of the zoom lens system in the wide-angle end,and ih denotes a maximum image height in an effective image takingregion of the light receiving surface.

In the present invention, a fourth type of image taking apparatuscomprises:

a zoom lens system; and

an image sensor which is disposed on an image side of the zoom lenssystem, which has a light receiving surface and which converts anoptical image formed by the zoom lens system into an electric signal,

the zoom lens system comprising, in order from an object side:

a first lens unit having a positive refractive power; a second lens unithaving a negative refractive power; a third lens unit having a positiverefractive power; a fourth lens unit having a negative refractive power;and a fifth lens unit having a positive refractive power,

the zoom lens system having five lens units in total,

during zooming from a wide-angle end toward a telephoto end, the firstlens unit being fixed, at least the second lens unit and the third lensunit being moved, and a space between the lens units being changed,

the second lens unit being positioned closer to an image-surface side inthe telephoto end than in the wide-angle end,

the third lens unit being positioned closer to the object side in thetelephoto end than in the wide-angle end,

the first lens unit comprising a reflective optical element whichreflects an optical path,

the apparatus satisfying the following conditions:

1.5<f _(w) /ih<1.9  (6B);

0.85<|f _(2G) /ih|<3.23  (8B);

1.0<f _(3G) /ih<3.7  (17B); and

0.6<m _(2GZ) /m _(3GZ)<1.4  (3B),

wherein f_(w) denotes a focal length of the zoom lens system in thewide-angle end, f_(2G) denotes a focal length of the second lens unit,f_(3G) denotes a focal length of the third lens unit, ih denotes amaximum image height in an effective image taking region of the lightreceiving surface, m_(2GZ) denotes a ratio of a magnification of thesecond lens unit in the telephoto end to that in the wide-angle end whenthe zoom lens system is focused on an infinite object, and M_(3GZ)denotes a ratio of a magnification of the third lens unit in thetelephoto end to that in the wide-angle end when the zoom lens system isfocused on the infinite object.

Other characteristics and advantages of the present invention will beapparent by embodiments described hereinafter with reference to thedrawings and description of appended claims.

BRIEF DESCRIPTION OF THE DRAWINGS

FIGS. 1A to 1C are sectional views showing a lens arrangement, along anextended line, in Example 1 of an optical path bending type zoom lenssystem in the present invention when focused on an infinite object, FIG.1A shows a wide-angle end, FIG. 1B shows an intermediate state, and FIG.1C shows a telephoto end;

FIGS. 2A to 2C are sectional views showing a lens arrangement, along anextended line, in Example 2 of an optical path bending type zoom lenssystem in the present invention when focused on an infinite object, FIG.2A shows a wide-angle end, FIG. 2B shows an intermediate state, and FIG.2C shows a telephoto end;

FIGS. 3A to 3C are sectional views showing a lens arrangement, along anextended line, in Example 3 of an optical path bending type zoom lenssystem in the present invention when focused on an infinite object, FIG.3A shows a wide-angle end, FIG. 3B shows an intermediate state, and FIG.3C shows a telephoto end;

FIGS. 4A to 4C are sectional views showing a lens arrangement, along anextended line, in Example 4 of an optical path bending type zoom lenssystem in the present invention when focused on an infinite object, FIG.4A shows a wide-angle end, FIG. 4B shows an intermediate state, and FIG.4C shows a telephoto end;

FIG. 5 is a sectional view showing a lens arrangement in a state inwhich an optical path of Example 1 shown in FIG. 1A is bent;

FIGS. 6A to 6C are aberration diagrams during the focusing on theinfinitely far object point in Example 1, FIG. 6A shows a wide-angleend, FIG. 6B shows an intermediate state, and FIG. 6C shows a telephotoend;

FIGS. 7A to 7C are aberration diagrams when focused on the infiniteobject in Example 2, FIG. 7A shows a wide-angle end, FIG. 7B shows anintermediate state, and FIG. 7C shows a telephoto end;

FIGS. 8A to 8C are aberration diagrams when focused on the infiniteobject in Example 3, FIG. 8A shows a wide-angle end, FIG. 8B shows anintermediate state, and FIG. 8C shows a telephoto end;

FIGS. 9A to 9C are aberration diagrams when focused on the infiniteobject in Example 4, FIG. 9A shows a wide-angle end, FIG. 9B shows anintermediate state, and FIG. 9C shows a telephoto end;

FIGS. 10A to 10C are sectional views showing a lens arrangement, alongan extended line, in Example 5 of an optical path bending type zoom lenssystem in the present invention when focused on an infinite object, FIG.10A shows a wide-angle end, FIG. 10B shows an intermediate state, andFIG. 10C shows a telephoto end;

FIGS. 11A to 11C are sectional views showing a lens arrangement, alongan extended line, in Example 6 of an optical path bending type zoom lenssystem in the present invention when focused on an infinite object, FIG.11A shows a wide-angle end, FIG. 11B shows an intermediate state, andFIG. 11C shows a telephoto end;

FIGS. 12A to 12C are sectional views showing a lens arrangement, alongan extended line, in Example 7 of an optical path bending type zoom lenssystem in the present invention when focused on an infinite object, FIG.12A shows a wide-angle end, FIG. 12B shows an intermediate state, andFIG. 12C shows a telephoto end;

FIG. 13 is a sectional view showing a lens arrangement in a state inwhich an optical path of Example 5 shown in FIG. 10A is bent;

FIGS. 14A to 14C are aberration diagrams when focused on the infiniteobject in Example 5, FIG. 14A shows a wide-angle end, FIG. 14B shows anintermediate state, and FIG. 14C shows a telephoto end;

FIGS. 15A to 15C are aberration diagrams when focused on the infiniteobject in Example 6, FIG. 15A shows a wide-angle end, FIG. 15B shows anintermediate state, and FIG. 15C shows a telephoto end;

FIGS. 16A to 16C are aberration diagrams when focused on the infiniteobject in Example 7, FIG. 16A shows a wide-angle end, FIG. 16B shows anintermediate state, and FIG. 16C shows a telephoto end;

FIG. 17 is a front perspective view showing an appearance of a digitalcamera in which the optical path bending type zoom lens system of thepresent invention is incorporated;

FIG. 18 is a rear perspective view of the digital camera of FIG. 17;

FIG. 19 is a sectional view of the digital camera of FIG. 17; and

FIG. 20 is a diagram showing one example of a pixel arrangement of animage sensor.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT

As described above, in the present invention, a first type of zoom lenssystem comprises, in order from an object side: a first lens unit havinga positive refractive power; a second lens unit having a negativerefractive power; a third lens unit having a positive refractive power;and a fourth lens unit having a positive refractive power. The zoom lenssystem has four lens units in total.

During zooming from a wide-angle end toward a telephoto end, the firstlens unit is fixed, at least the second lens unit and the third lensunit move, and a space between the third lens unit and the fourth lensunit changes. The second lens unit is positioned closer to animage-surface side in the telephoto end than in the wide-angle end. Thethird lens unit is positioned closer to the object side in the telephotoend than in the wide-angle end. The first lens unit comprises areflective optical element which reflects an optical path.

The zoom lens system satisfies the following condition:

0.5<f _(1G) /f _(w)<3.5  (1A),

wherein f_(1G) denotes a focal length of the first lens unit, and f_(w)denotes a focal length of the zoom lens system in the wide-angle end.

The above zoom lens system includes, in order from an object, fourpositive, negative, positive, and positive lens units. Moreover, thepositive first lens unit includes the reflective optical element, and athin zoom lens system is constituted in which the optical path is bentby the reflection. The zooming is performed mainly by moving the secondlens unit and the third lens unit.

At this time, when a zooming function is performed mainly by the secondlens unit, a movement amount of the second lens unit increases. Thiseasily increases the height of an off-axial ray incident upon the firstlens unit. Therefore, it becomes difficult to reduce a lens diameter ofthe first lens unit.

To solve the problem, in this zoom lens system, the third lens unit isalso provided with a zooming function, and a burden of the zoomingfunction imposed on the second lens unit is reduced. Accordingly, themovement amount of the second lens unit is reduced. Therefore, a heightof ray in the first lens unit can be reduced.

Moreover, in this zoom lens system, the positive power of the first lensunit is set so as to satisfy the condition (1A). In consequence, thelens of the first lens unit can be miniaturized to reduce a bentthickness of the zoom lens system.

Below the lower limit of 0.5 of the condition (1A), the power of thefirst lens unit is strengthened, and this is advantageous inminiaturizing the first lens unit. However, in the first lens unit, alarge spherical aberration or astigmatism is generated, and it becomesdifficult to correct aberrations of the whole lens system.

On the other hand, above the upper limit of 3.5 of the condition (1A),the power of the first lens unit weakens, the movement amount of thesecond lens unit increases, and the first lens unit is easily enlargedin size. Alternatively, the positive refractive power of the third lensunit is strengthened, and it becomes difficult to reduce, with fewerlenses, aberration fluctuations generated by the movement of the thirdlens unit.

When the following constitutions are introduced in addition to the abovebasic constitution, a more satisfactory zoom lens system can beobtained.

The above zoom lens system preferably satisfies the following condition:

0.5<|f _(2G) /f _(w)|<1.8  (2A),

wherein f_(2G) is a focal length of the second lens unit.

The condition (2A) appropriately defines the power of the second lensunit. If the condition (2A) is below the lower limit of 0.5, and thepower of the second lens unit is strengthened, the movement amount ofthe second lens unit decreases, and this is advantageous in reducing atotal length. However, the astigmatism or a distortion is easilygenerated, and it becomes difficult to correct the aberrations of thewhole lens system.

Above the upper limit of 1.8 in the condition (2A), the movement amountof the second lens unit excessively increases, and it becomes difficultto shorten the total length.

Moreover, the above zoom lens system preferably satisfies the followingcondition:

0.7<m _(2GZ) /m _(3GZ)<1.2  (3A),

wherein m_(2GZ) denotes a ratio of a magnification of the second lensunit in the telephoto end to that in the wide-angle end when the zoomlens system is focused on an infinite object, and M_(3GZ) denotes aratio of a magnification of the third lens unit in the telephoto end tothat in the wide-angle end when the zoom lens system is focused on theinfinite object.

The condition (3A) appropriately defines the burden of the zoomingfunction shared by the second lens unit and the third lens unit. Abovethe upper limit of 1.2 in the condition (3A), the burden of the zoomingfunction share by the second lens unit increases, and the movementamount of the second lens unit increases. Therefore, the diameter of thefirst lens unit easily becomes large. Alternatively, the refractivepower of the second lens unit increases, and the aberration fluctuationsby the movement of the second lens unit are not easily reduced.

Below the lower limit of 0.7 in the condition (3A), the burden of thezooming function shared by the third lens unit increases, and themovement amount of the third lens unit easily increases. Therefore, thetotal length easily increases. Alternatively, the refractive power ofthe third lens unit increases, and the aberration fluctuations by themovement of the third lens unit are not easily reduced.

Furthermore, the above zoom lens system preferably satisfies thefollowing condition:

−0.2<f _(w) /R ₁<0.2  (4A),

wherein R₁ denotes a paraxial radius of curvature of an object-sidesurface of the lens closest to the object side in the first lens units.

The condition (4A) defines the paraxial radius of curvature of theobject-side surface of the lens closest to the object side in the firstlens unit. Below the lower limit of −0.2, a large negative distortion iseasily generated in the wide-angle end.

Above the upper limit of 0.2 in the condition (4A), an off-axialaberration is advantageously corrected. On the other hand, a vertex of alens surface easily protrudes toward the object side, and it becomesdifficult to constitute the system to be thin.

Moreover, in the above zoom lens system, the first lens unit ispreferably constituted of, in order from the object side, a negativemeniscus lens directing its convex surface on the object side, areflective optical element for bending the optical path, and a positivesub-unit.

When the first lens unit is provided with the reflective optical elementfor bending the optical path, there inevitably arises a tendency todeepen an entrance pupil position. Therefore, a diameter or a size ofeach optical element constituting the first lens unit increases, and theoptical path bending type system is not physically easily established.Therefore, the first lens unit is constituted of, in order from theobject side, the negative meniscus lens directing its convex surface onthe object side, the reflective optical element for bending the opticalpath, and the positive sub-unit. According to this constitution, a chiefray becomes nearly parallel with the optical axis in the space requiredfor disposing the reflective optical element, and this can inhibit theincrease of the diameter of the optical element.

To miniaturize the image taking apparatus in the height direction or thelateral direction, it is preferable that the positive sub-unit isconstituted of one positive lens.

Furthermore, the first lens unit may be constituted of, in order fromthe object side, a negative sub-unit, a reflective optical element forbending the optical path, and a positive sub-unit so that the negativesub-unit satisfies the following condition:

0.5<|f _(L1) /f _(w)|<2.5  (5A),

wherein f_(L1) denotes a focal length of the negative sub-unit of thefirst lens unit.

To constitute the entrance pupil to be shallow so that the optical pathcan physically be bent, the power of the negative sub-unit of the firstlens unit may be set to be appropriately strong as in the condition(5A).

Above the upper limit of 2.5 in the condition (5A), the entrance pupilremains to be deep. Therefore, when an angle of field is secured to acertain degree, the diameter or the size of each optical elementconstituting the first lens unit increases, and the optical path is notphysically easily bent.

Below the lower limit of 0.5 in the condition (5A), the magnification ofthe lens unit or lens units, which are disposed subsequently to thefirst lens unit and being constituted to move for the zooming, comesclose to zero. This easily generates a problem such that the movementamount increases or the zooming ratio decreases. Moreover, it becomesdifficult to correct an off-axial aberration such as distortion, or achromatic aberration.

In the above zoom lens system, focusing on an object at a short distancemay be performed only by moving the fourth lens unit toward the objectside.

When the fourth lens unit is moved toward the object side to perform thefocusing, there are preferably less fluctuations of the off-axialaberration at the short distance.

In a case where the zoom lens system is used as a photographing opticalsystem of the image taking apparatus, it is preferable that an imagesensor is disposed on the image side of the zoom lens system, the imagesensor having a light receiving surface and converting an optical imageformed by the zoom lens system into an electric signal. Furthermore, thefollowing condition is preferably satisfied:

1.6<f _(w) /ih<1.9  (6A),

wherein ih denotes a maximum image height in an effective image takingregion of the light receiving surface.

The condition (6A) defines the focal length of the zoom lens system withrespect to the maximum image height in the wide-angle end. Below thelower limit of 1.6 in the condition (6A), the angle of field in thewide-angle end is reduced, and this is contrary to a purpose ofenlarging the angle of field.

On the other hand, above the upper limit of 1.9, the angle of fieldbecomes excessively large. To secure the bent optical path, thethickness of the zoom lens system is increased.

This condition (6A) defines the range of the focal length f_(w) in thewide-angle end in the condition (1A) or the like.

It is to be noted that the effective image taking region of the lightreceiving surface means a region for obtaining image information for usein printing or displaying an image. The region is disposed on the lightreceiving surface of the image sensor which receives the optical imageformed by the zoom lens system.

In a case where the effective image taking region of the image sensor isrectangular, and the optical axis of the zoom lens system passes throughthe center of the effective image taking region, the maximum imageheight ih in the effective image taking region of the light receivingsurface is ½ of a diagonal length L of the effective image takingregion. The diagonal length L of the effective image taking region willbe described. FIG. 20 is a diagram showing one example of a pixelarrangement on the light receiving surface of the image sensor. In thisexample, red (R), green (G) and blue (B) pixels are arranged at an equalpitch in a mosaic form. The effective image taking region means a regionin the light receiving surface of the image sensor for use inreproducing photographed image (displaying the image in a personalcomputer, printing the image by a printer or the like).

As shown in, for example, FIG. 20, an effective image taking region EIis sometimes set to be smaller than the whole light receiving surface ofthe image sensor in accordance with a performance of the optical system.For example, in an image (image circle) obtained by the optical system,the image quality of the peripheral portion is inferior to that of thecenter in many cases. In such case, as an example in which the region isset to be small, a part of the peripheral portion of the image circle isnot used in reproducing the image. The diagonal length L of theeffective image taking region is a diagonal length of this effectiveimage taking region. It is to be noted that an image taking region foruse in reproducing the video can be variously changed, and the maximumimage height ih in the effective image taking region changes, in a casewhere the above zoom lens system is used in the image taking apparatushaving such function. In such case, it is assumed that the effectiveimage taking region which defines the maximum image height ih is aneffective image taking region where ih is maximized.

The above zoom lens system has a wide angle, and is advantageous inreducing the thickness or the total length.

The zoom lens system has been described above in detail, and the imagetaking apparatus has been briefly described in which the zoom lenssystem is combined with the image sensor. Next, there will be describedin more detail the image taking apparatus including the optical pathbending type zoom lens system and the image sensor.

In the present invention, a first type of image taking apparatuscomprises:

a zoom lens system; and an image sensor which is disposed on an imageside of the zoom lens system, which has a light receiving surface andwhich converts an optical image formed by the zoom lens system into anelectric signal.

The zoom lens system comprises, in order from an object side: a firstlens unit having a positive refractive power; a second lens unit havinga negative refractive power; a third lens unit having a positiverefractive power; and a fourth lens unit having a positive refractivepower. The zoom lens system has four lens units in total.

During zooming from a wide-angle end toward a telephoto end, the firstlens unit is fixed to an image surface on the light receiving surface,at least the second lens unit and the third lens unit move, and a spacebetween the third lens unit and the fourth lens unit changes. The secondlens unit is positioned closer to an image-surface side in the telephotoend than in the wide-angle end. The third lens unit is positioned closerto the object side in the telephoto end than in the wide-angle end. Thefirst lens unit comprises a reflective optical element which reflects anoptical path.

The apparatus satisfies the following conditions:

1.6<f _(w) /ih<1.9  (6A); and

0.85<f _(1G) /ih<6.0  (7A),

wherein f_(1G) denotes a focal length of the first lens unit, f_(w)denotes a focal length of the zoom lens system in the wide-angle end,and ih denotes a maximum image height in an effective image takingregion of the light receiving surface.

The condition (6A) defines a relation between the focal length and themaximum image height of the effective image taking region in thewide-angle end. Below the lower limit of 1.6 in the condition (6A), theangle of field in the wide-angle end is unfavorably reduced.

On the other hand, above the upper limit of 1.9 in the condition (6A),the angle of field becomes excessively large. To secure the bent opticalpath, the thickness of the zoom lens system is increased.

The condition (7A) defines a relation between the focal length of thefirst lens unit and the maximum image height. The purpose of setting thecondition is similar to that of setting the condition (1A). If thecondition (7A) is below the lower limit of 0.85, and the power of thefirst lens unit is strengthened, the first lens unit is advantageouslyminiaturized. However, a spherical aberration or astigmatism is largelygenerated in the first lens unit, and it becomes difficult to correctthe aberration of the whole lens system.

On the other hand, above the upper limit of 6.0 in the condition (7A),the power of the first lens unit weakens, the movement amount of thesecond lens unit increases, and the first lens unit is easily enlargedin size. Alternatively, the positive refractive power of the third lensunit is strengthened, and it becomes difficult to reduce, with fewerlenses, aberration fluctuations generated by the movement of the thirdlens unit.

The image taking apparatus preferably satisfies the following condition:

0.85<|f _(2G) /ih|<3.1  (8A),

wherein f_(2G) denotes a focal length of the second lens unit.

The condition (8A) defines a relation between the power of the secondlens unit and the maximum image height. The purpose of setting thecondition is similar to that of setting the condition (2A). If thecondition (8A) is below the lower limit of 0.85, and the power of thesecond lens unit is strengthened, the movement amount of the second lensunit decreases. This is advantageous in reducing the total length of thezoom lens system. However, astigmatism or a distortion is largelygenerated, and it becomes difficult to correct the aberration of thewhole lens system.

Above the upper limit of 3.1 in the condition (8A), the movement amountof the second lens unit becomes excessively large, and it becomesdifficult to shorten the total length.

Moreover, it is preferable that the above image taking apparatussatisfies the following condition:

0.7<m _(2GZ) /m _(3GZ)<1.2  (3A),

wherein m_(2GZ) denotes a ratio of the magnification of the second lensunit in the telephoto end to that in the wide-angle end when the zoomlens system is focused on an infinite object, and M_(3GZ) denotes aratio of the magnification of the third lens unit in the telephoto endto that in the wide-angle end when the zoom lens is focused on theinfinite object.

The reason for the above constitution and the function and the effect ofthe constitution are as described above.

Moreover, it is preferable that the above image taking apparatussatisfies the following condition:

−0.118<ih/R ₁<0.118  (9A),

wherein R₁ denotes a paraxial radius of curvature of the object-sidesurface of a lens closest to the object side in the first lens unit.

The condition (9A) defines a relation between the paraxial radius ofcurvature of the object-side surface of the lens closest to the objectside in the first lens unit and the maximum image height. The purpose ofsetting the condition is similar to that of setting the condition (4A).Below the lower limit of −0.118 in the condition (9A), a large negativedistortion is easily generated in the wide-angle end.

Above the upper limit value of 0.118 in the condition (9A), an off-axialaberration is advantageously corrected. However, the vertex of the lenssurface easily protrudes toward the object side, and it becomesdifficult to constitute the system to be thin.

Moreover, in the above image taking apparatus, the first lens unit ofthe zoom lens system includes, in order from the object side, a negativemeniscus lens directing its convex surface on the object side, areflective optical element for bending the optical path, and a positivesub-unit.

The reason for the above constitution and the function and the effect ofthe constitution are as described above.

Furthermore, the first lens unit may be constituted of, in order fromthe object side, a negative sub-unit, a reflective optical element forbending the optical path, and a positive sub-unit so that the negativesub-unit satisfies the following condition:

0.85<|f _(L1) /ih|<4.25  (10A),

wherein f_(L1) denotes a focal length of the negative sub-unit of thefirst lens unit.

The condition (10A) defines a relation between the focal length of thenegative sub-unit constituting a front sub-unit of the first lens unitand the maximum image height. The purpose of setting the condition issimilar to that of the condition (5A), and the power of the negativesub-unit of the first lens unit may be appropriately strengthened.

Above the upper limit of 4.25 in the condition (10A), the entrance pupilremains to be deep. Therefore, when the angle of field is secured to acertain degree, the diameter or the size of each optical elementconstituting the first lens unit increases, and the optical path is notphysically easily bent.

Below the lower limit of 0.85 in the condition (10A), the magnificationof the lens unit or lens units, which are disposed subsequently to thefirst lens unit and are constituted to move for the zooming, comes closeto zero. This easily generates a problem such that the movement amountincreases or the zooming ratio decreases. Moreover, it becomes difficultto correct an off-axial aberration such as the distortion, or achromatic aberration.

To miniaturize the image taking apparatus in the thickness direction,the negative sub-unit is preferably constituted of a single lens.

To miniaturize the image taking apparatus in the height direction or thelateral direction, the positive sub-unit is preferably constituted of asingle lens.

Moreover, in the above image taking apparatus, the fourth lens unit maybe moved toward the object side to thereby focus on an object at a shortdistance.

The reason for the constitution and the function and the effect of theconstitution are as described above.

Furthermore, in the above image taking apparatus, it is preferable thatthe positive sub-unit of the first lens unit of the zoom lens systemsatisfies the following condition:

1.5<f _(L2) /ih<4.0  (11A),

wherein f_(L2) denotes a focal length of the positive sub-unit of thefirst lens unit.

The condition (11A) defines a relation between the focal length of thepositive sub-unit constituting a rear sub-unit of the first lens unitand the maximum image height. The power of the negative sub-unit of thefirst lens unit may appropriately be strengthened. In this case, anoff-axial aberration such as the distortion is easily generated.Therefore, when an appropriately strong power is also imparted to thepositive sub-unit disposed close to the negative sub-unit, theaberration is easily prevented from being generated. This is alsoadvantageous in constituting the first lens unit to be compact.

Above the upper limit of 4.0 in the condition (11A), the power of thepositive sub-unit is reduced. This is disadvantageous in sufficientlycorrecting the off-axial aberration.

Below the lower limit of 1.5 in the condition (11A), the power of thepositive sub-unit becomes excessively strong, and it becomes difficultto correct the aberration of this lens unit.

In the above image taking apparatus, it is preferable to dispose anaperture stop between the second lens unit and the third lens unit.

This constitution is advantageous in substantially disposing the exitpupil at infinity while balancing the size of the whole lens system,that is, in constituting the whole lens system as an image-sidetelecentric optical system.

In a case where the aperture stop is disposed, the followingconstitution is especially preferable.

That is, it is preferable that the position of the aperture stop in thewide-angle end satisfies the following condition:

0.5<D _(2GS) /D _(S3G)<1.0  (12A),

wherein D_(2GS) denotes an axial length from the second lens unit to theaperture stop in the wide-angle end, and D_(S3G) denotes an axial lengthfrom the aperture stop to the third lens unit in the wide-angle end.

When the aperture stop is disposed close to the first lens unit and thesecond lens unit in the wide-angle end, the light beam transmittedthrough the first lens unit can be lowered. If the condition (12A) isbelow the lower limit of 0.5, and the aperture stop is separated fromthe third lens unit, the outer diameter of the third lens unit easilyincreases, and it becomes difficult to correct the aberration of thethird lens unit.

If the condition (12A) is above the upper limit of 1.0, and the aperturestop is separated from the second lens unit, it becomes difficult tominimize the first lens unit.

Moreover, in the above image taking apparatus, it is preferable that anaperture stop is disposed between the second lens unit and the thirdlens unit, the surface closest to the image side in the third lens unitis a concave surface, and the following condition is satisfied:

0.5<D _(2GS) /D _(S3G)<1.0  (12A); and

0.5<R _(3GE) /ih<2.5  (13A),

wherein D_(2GS) denotes an axial length from the second lens unit to theaperture stop in the wide-angle end, D_(S3G) denotes an axial lengthfrom the aperture stop to the third lens unit in the wide-angle end, andR_(3GE) denotes a paraxial radius of curvature of the concave surfaceclosest to the image side in the third lens unit.

An absolute value of the radius of curvature of the surface closest tothe object side in the first lens unit is reduced, or the power of thefront sub-unit having a negative refractive power is strengthened. Thisis advantageous in reducing the thickness of the first lens unit. On theother hand, an off-axial aberration is easily generated in thewide-angle end.

The condition (12A) specifies the position of the aperture stop asdescribed above. When this condition is satisfied, an incidence heightof a ray upon the first lens unit is advantageously lowered. This alsoincreases the incidence height of the ray upon the concave surface asthe exit surface of the third lens unit having a positive refractivepower. Therefore, the concave surface can be provided with an effect ofcorrecting the off-axial aberration.

The condition (13A) defines the paraxial radius of curvature of thisconcave surface. If the condition (13A) is below the lower limit of 0.5,the power of the concave surface becomes excessively strong. This isdisadvantageous in correcting the aberration of the third lens unititself. Above the upper limit of 2.5, the power of the concave surfaceweakens, and the function of correcting the off-axial aberration isdegraded.

Moreover, in the image taking apparatus, it is preferable that thefourth lens unit satisfies the following condition:

3.3<f _(4G) /ih<6.6  (14A),

wherein f_(4G) denotes a focal length of the fourth lens unit.

The condition (14A) defines a relation between the appropriaterefractive power of the fourth lens unit and the maximum image height.The fourth lens unit is disposed close to the image surface. Therefore,if the condition (14A) is below the lower limit of 3.3, and the power isexcessively strengthened, the aberration is easily generated, the lensesare increased in number, and the system is easily enlarged in size. Onthe other hand, if the condition is above the upper limit of 6.6, andthe power is excessively weak, it becomes difficult to securetelecentricity, or the space between the third lens unit and the fourthlens unit lengthens. This is disadvantageous in miniaturizing thesystem.

In the present invention, a second type of image taking apparatuscomprises:

a zoom lens system; and an image sensor which is disposed on an imageside of the zoom lens system, which has a light receiving surface andwhich converts an optical image formed by the zoom lens system into anelectric signal.

The zoom lens system comprises, in order from an object side: a firstlens unit having a positive refractive power; a second lens unit havinga negative refractive power; a third lens unit having a positiverefractive power; and a fourth lens unit having a positive refractivepower. The zoom lens system has four lens units in total.

During zooming from a wide-angle end toward a telephoto end, the firstlens unit is fixed, at least the second lens unit and the third lensunit move, and a space between the third lens unit and the fourth lensunit changes. The second lens unit is positioned closer to animage-surface side in the telephoto end than in the wide-angle end. Thethird lens unit is positioned closer to the object side in the telephotoend than in the wide-angle end. The first lens unit comprises areflective optical element which reflects an optical path.

The apparatus satisfies the following conditions:

1.6<f _(w) /ih<1.9  (6A);

0.85<|f _(2G) /ih|<3.1  (8A);

1.0<f _(3G) /ih<3.7  (15A); and

0.7<m _(2GZ) /m _(3GZ)<1.2  (3A),

wherein f_(w) denotes a focal length of the whole zoom lens system inthe wide-angle end, f_(2G) denotes a focal length of the second lensunit, f_(3G) denotes a focal length of the third lens unit, ih denotes amaximum image height in an effective image taking region of the lightreceiving surface, m_(2GZ) denotes a ratio of a magnification of thesecond lens unit in the telephoto end to that in the wide-angle end whenthe zoom lens system is focused on an infinite object, and M_(3GZ)denotes a ratio of a magnification of the third lens unit in thetelephoto end to that in the wide-angle end when the zoom lens system isfocused on the infinite object.

This image taking apparatus is advantageous in achieving miniaturizationand enhancement of the zooming ratio of the zoom lens system whoseoptical path is bent while securing an angle of field.

The zoom lens system for use herein is a thin zoom lens constituted offour lens units including, in order from the object side, positive,negative, positive, and positive lens units. In the positive first lensunit, the optical path is bent by reflection. Moreover, the second lensunit and the third lens unit are constituted to perform movement whichcontributes to the zooming.

At this time, when the second lens unit largely contributes to thezooming function, the movement amount of the second lens unit increases.An incidence height of an off-axial ray upon the first lens unit easilyincreases in the wide-angle end, and it becomes difficult to reduce thelens diameter of the first lens unit.

Therefore, the third lens unit is also provided with the zoomingfunction in this zoom lens system, and the burden of the zoomingfunction imposed on the second lens unit is reduced, thereby reducingthe movement amount of the second lens unit.

Moreover, the focal lengths of the second and third lens units areappropriately set to miniaturize the optical system whose optical pathis bent.

The condition (6A) defines a relation between the focal length and themaximum image height of the effective image taking region in thewide-angle end. Below the lower limit of 1.6 in the condition (6A), theangle of field in the wide-angle end is unfavorably reduced. On theother hand, above the upper limit of 1.9 in the condition (6A), theangle of field becomes excessively large. To secure the bent opticalpath, the thickness of the zoom lens system is increased.

The condition (8A) defines a relation between the power of the secondlens unit and the maximum image height. The purpose of setting thecondition is similar to that of setting the condition (2A). If thecondition (8A) is below the lower limit of 0.85, and the power of thesecond lens unit is strengthened, the movement amount of the second lensunit decreases. This is advantageous in reducing the total length of thezoom lens system. However, astigmatism or a distortion is largelygenerated, and it becomes difficult to correct the aberration of thewhole lens system.

Above the upper limit of 3.1 in the condition (8A), the movement amountof the second lens unit excessively increases, and it becomes difficultto shorten the total length.

The condition (15A) defines a relation between the power of the thirdlens unit and the maximum image height. If the condition (15A) is belowthe lower limit of 1.0, and the power of the third lens unit isstrengthened, the astigmatism or the distortion is largely generated,and it becomes difficult to correct the aberration of the whole lenssystem. Above the upper limit of 3.7 of the condition (15A), themovement amount of the third lens unit becomes excessively large, and itbecomes difficult to reduce the total length.

The condition (3A) appropriately defines the burden of the zoomingfunction shared by the second lens unit and the third lens unit. Abovethe upper limit of 1.2 in the condition (3A), the burden of the zoomingfunction shared by the second lens unit increases, and the movementamount of the second lens unit increases. Therefore, the diameter of thefirst lens unit easily becomes large. Alternatively, the refractivepower of the second lens unit increases, and the aberration fluctuationsby the movement of the second lens unit are not easily reduced.

Below the lower limit of 0.7 in the condition (3A), the burden of thezooming function shared by the third lens unit increases, and themovement amount of the third lens unit easily increases. Therefore, thetotal length easily increases. Alternatively, the refractive power ofthe third lens unit increases, and the aberration fluctuations by themovement of the third lens unit are not easily reduced.

Moreover, the following constitution is preferable in order tominiaturize the system and satisfactorily correct the aberration whileimposing the zooming burdens on the second and third lens units.

That is, the second lens unit is constituted of, in order from theobject side, a negative single lens having a smaller absolute value ofthe paraxial radius of curvature in an image-side surface than in anobject-side surface, and a cemented lens of a double-concave negativelens and a double-convex positive lens. The third lens unit isconstituted of, in order from the object side, a plurality of positivelenses, and one or two negative lenses. The positive lens and thenegative lens disposed adjacent to each other are cemented to constitutea cemented lens. The fourth lens unit is constituted of two lenses orone lens.

When the second lens unit includes, in order from the object side, twonegative lenses and the double-convex positive lens, the position of theprincipal point comes close to the object. This is advantageous inreducing diameters of the first and second lens units. When a mainnegative power of the second lens unit is shared by two negative lenses,the aberration can satisfactorily be corrected. Since the cemented lensof the negative lens and the double-convex positive lens is disposed, achromatic aberration of the second lens unit itself is easily corrected.

Moreover, a main positive power of the third lens unit is shared by aplurality of positive lenses. Furthermore, since the third lens unitincludes, in order from the object side, a plurality of positive lensesand one or two negative lenses, and the position of the principal pointis brought close to the object, the third lens unit can have a functionof increasing the focal length in the telephoto end.

Furthermore, when the third lens unit is provided with the cemented lensof the positive and negative lenses, the chromatic aberration is easilycorrected.

The fourth lens unit is positioned closest to the image surface in thezoom lens system. Therefore, when the number of lenses constituting thelens unit is reduced, the system is advantageously miniaturized. Thus,from a viewpoint of the miniaturization, it is preferable that thefourth lens unit is constituted of two lenses or one lens.

The above-described constitutions can be appropriately combined andintroduced into the image taking apparatus. Accordingly, effectsproduced by the constitutions can be obtained at the same time.

Furthermore, the image taking apparatus may be constituted to satisfy atleast one of the following constitutions.

That is, the image taking apparatus may be constituted to satisfy thefollowing condition:

0.85<f _(1G) /ih<6.0  (7A),

wherein f_(1G) denotes a focal length of the first lens unit.

Moreover, the image taking apparatus may be constituted to satisfy thefollowing condition:

−0.118<ih/R ₁<0.118  (9A),

wherein R₁ denotes a paraxial radius of curvature of an object-sidesurface of a lens closest to the object side in the first lens unit.

Furthermore, in the image taking apparatus, the first lens unit may beconstituted of, in order from the object side, a negative meniscus lensdirecting its convex surface on the object side, a reflective opticalelement for bending the optical path, and a positive sub-unit.

Furthermore, in the image taking apparatus, the first lens unit may beconstituted of, in order from the object side, a negative sub-unit, areflective optical element for bending the optical path, and a positivesub-unit so that the negative sub-unit satisfies the followingcondition:

0.85<|f _(L1) /ih|<4.25  (10A),

wherein f_(L1) denotes a focal length of the negative sub-unit of thefirst lens unit.

From a viewpoint of miniaturization, it is preferable that one or bothof the positive sub-unit and the negative sub-unit is constituted of asingle lens.

Moreover, the positive sub-unit of the first lens unit may beconstituted to satisfy the following condition:

1.5<f _(L2) /ih<4.0  (11A),

wherein f_(L2) denotes a focal length of the positive sub-unit of thefirst lens unit.

Furthermore, the image taking apparatus may be constituted so as todispose an aperture stop between the second lens unit and the third lensunit.

In the wide-angle end, the aperture stop is preferably disposed in aposition which satisfies the following condition:

0.5<D _(2GS) /D _(S3G)<1.0  (12A),

wherein D_(2GS) denotes an axial length from the second lens unit to theaperture stop in the wide-angle end, and D_(S3G) denotes an axial lengthfrom the aperture stop to the third lens unit in the wide-angle end.

Moreover, in the image taking apparatus, an aperture stop is disposedbetween the second lens unit and the third lens unit, and the surfaceclosest to the image side in the third lens unit is a concave surfacewhich can be constituted to satisfy the following conditions:

0.5<D _(2GS) /D _(S3G)<1.0  (12A); and

0.5<R _(3GE) /ih<2.5  (13A),

wherein D_(2GS) denotes an axial length from the second lens unit to theaperture stop in the wide-angle end, D_(S3G) denotes an axial lengthfrom the aperture stop to the third lens unit in the wide-angle end, andR_(3GE) denotes a paraxial radius of curvature of the concave surfaceclosest to the image side in the third lens unit.

Moreover, in the image taking apparatus, the fourth lens unit may beconstituted to satisfy the following condition:

3.3<f _(4G) /ih<6.6  (14A),

wherein f_(4G) denotes a focal length of the fourth lens unit.

The upper and lower limit values of the above conditions (1A) to (15A)can be changed as follows.

As to the condition (1A), the lower limit value is more preferably setto 1.0, further 1.5, and the upper limit value is more preferably set to3.0, further 2.5.

As to the condition (2A), the lower limit value is more preferably setto 0.8, further 1.3, and the upper limit value is more preferably set to1.6, further 1.5.

As to the condition (3A), the lower limit value is more preferably setto 0.75, further 0.77, and the upper limit value is more preferably setto 1.1, further 1.05.

As to the condition (4A), the lower limit value is more preferably setto −0.1, further −0.05, and the upper limit value is more preferably setto 0.15, further 0.1.

As to the condition (5A), the lower limit value is more preferably setto 1.0, further 1.5, and the upper limit value is more preferably set to2.2, further 2.0.

As to the condition (6A), the lower limit value is more preferably setto 1.63, further 1.66, and the upper limit value is more preferably setto 1.8, further 1.75.

As to the condition (7A), the lower limit value is more preferably setto 1.7, further 2.55, and the upper limit value is more preferably setto 5.1, further 4.25.

As to the condition (8A), the lower limit value is more preferably setto 1.36, further 2.21, and the upper limit value is more preferably setto 2.72, further 2.55.

As to the condition (9A), the lower limit value is more preferably setto −0.059, further −0.029, and the upper limit value is more preferablyset to 0.088, further 0.059.

As to the condition (10A), the lower limit value is more preferably setto 1.7, further 2.55, and the upper limit value is more preferably setto 3.74, further 3.4.

As to the condition (11A), the lower limit value is more preferably setto 1.8, further 2.2, and the upper limit value is more preferably set to3.5, further 3.0.

As to the condition (12A), the lower limit value is more preferably setto 0.6, further 0.65, and the upper limit value is more preferably setto 0.95, further 0.9.

As to the condition (13A), the lower limit value is more preferably setto 0.7, further 0.9, and the upper limit value is more preferably set to2.0, further 1.5.

As to the condition (14A), the lower limit value is more preferably setto 3.5, further 3.7, and the upper limit value is more preferably set to5.5, further 5.3.

As to the condition (15A), the lower limit value is more preferably setto 2.0, further 2.5, and the upper limit value is more preferably set to3.4, further 3.1.

It is to be noted that the above constitutions or conditions areappropriately combined to produce effects. Therefore, they are moreeffective.

The above-described optical path bending type zoom lens system and theimage taking apparatus are small in the thickness direction. Moreover,the angle of field can sufficiently be secured. The bent constitution isminiaturized while obtaining a large angle of field. In consequence, thesize of the image taking apparatus can be reduced in the heightdirection or the lateral direction.

Next, there will be described numerical examples of the first type ofoptical path bending type zoom lens system.

FIGS. 1A to 4C show lens sectional views when the zoom lens system isfocused on an infinite object in Examples 1 to 4. In these drawings,FIGS. 1A, 2A, 3A and 4A are lens sectional views in a wide-angle end.FIGS. 1B, 2B, 3B and 4B are lens sectional views in an intermediatestate. FIGS. 1C, 2C, 3C and 4C are lens sectional views in a telephotoend. In these drawings: the first lens unit is denoted with G1; thesecond lens unit is denoted with G2; the aperture stop is denoted withS; the third lens unit is denoted with G3; the fourth lens unit isdenoted with G4; F denotes an optical low pass filter having an IR cutcoating surface; C denotes cover glass of the electronic image sensorsuch as a CCD image sensor or a CMOS image sensor; and the image surface(light receiving surface) of the CCD image sensor, the CMOS image sensoror the like is denoted with I. Moreover, P denotes an optical pathbending prism in the first lens unit G1, which is shown as a parallelflat plate developed on a straight optical axis. It is to be noted thatas shown, the surface of the optical low pass filter F may directly becoated with an IR cut coating, or an IR cutting absorbent filter mayseparately be disposed. Alternatively, a transparent flat plate whoseincidence surface is coated with the IR cut coating may be used.

FIG. 5 is a diagram showing a state in which the optical path of FIG. 1Ais bent. The optical path bending prism P is constituted of a reflectiveprism which bends the optical path by 90°. It is to be noted that inExamples 1 to 4, the reflection position is in the center between theincidence surface and the exit surface of the parallel flat plate P.Moreover, the reflecting direction of the optical path bending prism Pis a longitudinal direction (the vertical direction when the incidentoptical path is in the horizontal direction) of the image takingapparatus, and a short-side direction of the light receiving surface ofthe electronic image sensor. It is to be noted that the reflectingdirection may be a long-side direction of the light receiving surface.

As shown in FIGS. 1A to 1C, the zoom lens system of Example 1 isconstituted of, in order from an object side: a first lens unit G1having a positive refractive power; a second lens unit G2 having anegative refractive power; an aperture stop S; a third lens unit G3having a positive refractive power; and a fourth lens unit G4 having apositive refractive power. When zooming is performed from the wide-angleend toward the telephoto end, the first lens unit G1 is fixed, thesecond lens unit G2 moves toward an image surface, the aperture stop Sis substantially fixed, the third lens unit G3 moves toward the object,the fourth lens unit G4 moves along a locus concave toward the objectwhile broadening the space between the third lens unit G3 and the fourthlens unit, and the fourth lens unit is positioned closer to theimage-surface side in the telephoto end than in the wide-angle end.

The first lens unit G1 includes, in order from the object side, anegative meniscus lens directing its convex surface on the object side,an optical path bending prism P, and a double-convex positive lens. Thesecond lens unit G2 includes, in order from the object side, a negativemeniscus lens directing its convex surface on the object side, and acemented lens of a double-concave negative lens and a double-convexpositive lens. The third lens unit G3 includes, in order from the objectside, a double-convex positive lens and a cemented lens of a positivemeniscus lens directing its convex surface on the object side and anegative meniscus lens directing its convex surface on the object side.The fourth lens unit G4 includes, in order from the object side, anegative meniscus lens directing its convex surface on the object sideand a double-convex positive lens.

Aspherical surfaces are used on six surfaces: opposite surfaces of thedouble-convex positive lens of the first lens unit G1; opposite surfacesof the double-convex positive lens of the third lens unit G3; andopposite surfaces of the double-convex positive lens of the fourth lensunit G4.

As shown in FIGS. 2A to 2C, the zoom lens system of Example 2 isconstituted of, in order from an object side: a first lens unit G1having a positive refractive power; a second lens unit G2 having anegative refractive power; an aperture stop S; a third lens unit G3having a positive refractive power; and a fourth lens unit G4 having apositive refractive power. When zooming is performed from the wide-angleend toward the telephoto end, the first lens unit G1 is fixed, thesecond lens unit G2 moves toward the image surface, the aperture stop Sis fixed, the third lens unit G3 moves toward the object, and the fourthlens unit G4 moves toward the image surface while broadening the spacebetween the third lens unit G3 and the fourth lens unit.

The first lens unit G1 includes, in order from the object side, anegative meniscus lens directing its convex surface on the object side,an optical path bending prism P, and a double-convex positive lens. Thesecond lens unit G2 includes, in order from the object side, adouble-concave negative lens, and a cemented lens of a double-concavenegative lens and a double-convex positive lens. The third lens unit G3includes, in order from the object side, a double-convex positive lens,and a cemented lens of a double-convex positive lens and adouble-concave negative lens. The fourth lens unit G4 includes onedouble-convex positive lens.

Aspherical surfaces are used on six surfaces: opposite surfaces of thedouble-convex positive lens of the first lens unit G1; opposite surfacesof the double-convex positive lens of the third lens unit G3; andopposite surfaces of the double-convex positive lens of the fourth lensunit G4.

As shown in FIGS. 3A to 3C, the zoom lens system of Example 3 isconstituted of, in order from an object side: a first lens unit G1having a positive refractive power; a second lens unit G2 having anegative refractive power; an aperture stop S; a third lens unit G3having a positive refractive power; and a fourth lens unit G4 having apositive refractive power. When zooming is performed from the wide-angleend toward the telephoto end, the first lens unit G1 is fixed, thesecond lens unit G2 moves toward the image surface, the aperture stop Sis substantially fixed, the third lens unit G3 moves toward the object,and the fourth lens unit G4 moves toward the image surface whilebroadening the space between the third lens unit G3 and the fourth lensunit.

The first lens unit G1 includes, in order from the object side, adouble-concave negative lens, an optical path bending prism P, and adouble-convex positive lens. The second lens unit G2 includes, in orderfrom the object side, a negative meniscus lens directing its convexsurface on the object side, and a cemented lens of a double-concavenegative lens and a double-convex positive lens. The third lens unit G3includes, in order from the object side, two double-convex positivelenses, and a cemented lens of a double-convex positive lens and adouble-concave negative lens. The fourth lens unit G4 includes onedouble-convex positive lens.

Aspherical surfaces are used on six surfaces: opposite surfaces of thedouble-convex positive lens of the first lens unit G1; opposite surfacesof the double-convex positive lens arranged closest to the object in thethird lens unit G3; and opposite surfaces of the double-convex positivelens of the fourth lens unit G4.

As shown in FIGS. 4A to 4C, the zoom lens system of Example 4 isconstituted of, in order from an object side: a first lens unit G1having a positive refractive power; a second lens unit G2 having anegative refractive power; an aperture stop S; a third lens unit G3having a positive refractive power; and a fourth lens unit G4 having apositive refractive power. When zooming is performed from the wide-angleend toward the telephoto end, the first lens unit G1 is fixed, thesecond lens unit G2 moves toward the image surface, the aperture stop Sis fixed, the third lens unit G3 moves toward the object, the fourthlens unit G4 moves along a locus concave toward the object whilebroadening the space between the third lens unit G3 and the fourth lensunit, and the fourth lens unit is positioned closer to the image-surfaceside in the telephoto end than in the wide-angle end.

The first lens unit G1 includes, in order from the object side, anegative meniscus lens directing its convex surface on the object side,an optical path bending prism P, and a double-convex positive lens. Thesecond lens unit G2 includes, in order from the object side, adouble-concave negative lens, and a cemented lens of a double-concavenegative lens and a double-convex positive lens. The third lens unit G3includes, in order from the object side, a double-convex positive lens,a cemented lens of a double-convex positive lens and a double-concavenegative lens, and a negative meniscus lens directing its convex surfaceon the object side. The fourth lens unit G4 includes one double-convexpositive lens.

Aspherical surfaces are used on six surfaces: opposite surfaces of thedouble-convex positive lens of the first lens unit G1; opposite surfacesof the double-convex positive lens of the third lens unit G3; andopposite surfaces of the double-convex positive lens of the fourth lensunit G4.

There will be described hereinafter numeric value data of the aboveexamples. In addition to the above-described symbols: f denotes thefocal length of the zoom lens system; F_(NO) denotes the F number; ωdenotes a half angle of field; WE denotes a wide-angle end; ST denotesan intermediate state; TE denotes a telephoto end; r₁, r₂ . . . denote aradius of curvature of each lens surface; d₁, d₂ . . . denote a spacebetween the lens surfaces; n_(d1), n_(d2) . . . denote a refractiveindex of each lens for the wavelength of the d-line; and V_(d1), V_(d2). . . denote the Abbe number of each lens. It is to be noted that anaspherical shape is represented by the following equation in which x isan optical axis whose positive direction is set to the light travelingdirection, and y has a direction crossing the optical axis at rightangles:

x=(y ² /r)/[1+{1−(K+1)(y/r)²}^(1/2) ]+A ₄ y ⁴ +A ₆ y ⁶ +A ₈ y ⁸ +A ₁₀ y¹⁰,

wherein r denotes a paraxial radius of curvature, K denotes a coniccoefficient, and A₄, A₆, A₈ and A₁₀ denote fourth-order, sixth-order,eighth-order and tenth-order aspherical coefficients, respectively.

Example 1

TABLE 1 r₁ = 295.026 d₁ = 0.80 n_(d1) = 1.92286 V_(d1) = 20.88 r₂ =11.061 d₂ = 1.40 r₃ = ∞ d₃ = 7.40 n_(d2) = 1.83400 V_(d2) = 37.16 r₄ = ∞d₄ = 0.15 r₅ = 16.187* d₅ = 2.40 n_(d3) = 1.77377 V_(d3) = 47.17 r₆ =−15.754* d₆ = variable r₇ = 144.141 d₇ = 0.70 n_(d4) = 1.88300 V_(d4) =40.76 r₈ = 14.573 d₈ = 1.15 r₉ = −10.681 d₉ = 0.70 n_(d5) = 1.88300V_(d5) = 40.76 r₁₀ = 15.091 d₁₀ = 1.90 n_(d6) = 1.92286 V_(d6) = 20.88r₁₁ = −29.145 d₁₁ = (variable) r₁₂ = ∞ (AS) d₁₂ = (variable) r₁₃ =8.042* d₁₃ = 4.01 n_(d7) = 1.58313 V_(d7) = 59.46 r₁₄ = −22.780* d₁₄ =0.20 r₁₅ = 6.659 d₁₅ = 3.68 n_(d8) = 1.49700 V_(d8) = 81.54 r₁₆ = 74.227d₁₆ = 0.80 n_(d9) = 1.84666 V_(d9) = 23.78 r₁₇ = 4.449 d₁₇ = (variable)r₁₈ = 27.385 d₁₈ = 0.80 n_(d10) = 1.84666 V_(d10) = 23.78 r₁₉ = 12.421d₁₉ = 0.20 r₂₀ = 10.830* d₂₀ = 2.50 n_(d11) = 1.48749 V_(d11) = 70.23r₂₁ = −12.101* d₂₁ = (variable) r₂₂ = ∞ d₂₂ = 0.88 n_(d12) = 1.54771V_(d12) = 62.84 r₂₃ = ∞ d₂₃ = 0.89 r₂₄ = ∞ d₂₄ = 0.50 n_(d13) = 1.51633V_(d13) = 64.14 r₂₅ = ∞ d₂₅ = 0.60 r₂₆ = ∞ (IS) *Aspherical surface AS:Aperture stop IS: Image surface Aspherical Coefficient Fifth Surface K =0.000 A₄ = −8.31125 × 10⁻⁵ A₆ = −1.49859 × 10⁻⁷ A₈ = 1.31609 × 10⁻⁷ A₁₀= −6.10430 × 10⁻⁹ Sixth Surface K = 0.000 A₄ = −1.07939 × 10⁻⁵ A₆ =2.74948 × 10⁻⁶ A₈ = −1.35732 × 10⁻⁸ A₁₀ = −3.44642 × 10⁻⁹ 13th Surface K= 0.000 A₄ = 7.10303 × 10⁻⁶ A₆ = 5.21257 × 10⁻⁶ A₈ = 8.01135 × 10⁻⁷ A₁₀= −4.07370 × 10⁻⁸ 14th Surface K = 0.000 A₄ = 4.85355 × 10⁻⁴ A₆ =1.71401 × 10⁻⁵ A₈ = 2.37660 × 10⁻⁸ A₁₀ = 0 20th Surface K = 0.000 A₄ =−3.10795 × 10⁻⁴ A₆ = 2.67988 × 10⁻⁵ A₈ = 2.65967 × 10⁻⁸ A₁₀ = −1.19394 ×10⁻⁷ 21st Surface K = 0.000 A₄ = −4.20742 × 10⁻⁴ A₆ = 3.97404 × 10⁻⁵ A₈= 1.06118 × 10⁻⁹ A₁₀ = −1.23676 × 10⁻⁷

TABLE 2 Zoom Data (∞) WE ST TE f (mm) 6.898 11.557 19.670 F_(NO) 3.574.27 5.10 ω(°) 30.3 17.8 10.7 d₆ 0.50 3.71 5.73 d₁₁ 6.24 2.99 1.00 d₁₂7.21 5.05 1.20 d₁₇ 2.61 5.29 9.07 d₂₁ 3.12 2.66 2.67

Example 2

TABLE 3 r₁ = 92.883 d₁ = 0.80 n_(d1) = 1.92286 V_(d1) = 20.88 r₂ = 9.863d₂ = 1.75 r₃ = ∞ d₃ = 7.40 n_(d2) = 1.80100 V_(d2) = 34.90 r₄ = ∞ d₄ =0.16 r₅ = 14.947* d₅ = 2.67 n_(d3) = 1.77933 V_(d3) = 45.68 r₆ =−14.846* d₆ = variable r₇ = −39.260 d₇ = 0.80 n_(d4) = 1.88300 V_(d4) =40.76 r₈ = 17.909 d₈ = 0.73 r₉ = −18.959 d₉ = 0.70 n_(d5) = 1.87765V_(d5) = 40.94 r₁₀ = 11.087 d₁₀ = 1.70 n_(d6) = 1.92286 V_(d6) = 20.88r₁₁ = −122.735 d₁₁ = (variable) r₁₂ = ∞ (AS) d₁₂ = (variable) r₁₃ =7.900* d₁₃ = 3.68 n_(d7) = 1.58900 V_(d7) = 61.20 r₁₄ = −18.676* d₁₄ =0.15 r₁₅ = 8.530 d₁₅ = 4.35 n_(d8) = 1.49700 V_(d8) = 81.60 r₁₆ =−27.187 d₁₆ = 0.73 n_(d9) = 1.84666 V_(d9) = 23.78 r₁₇ = 4.740 d₁₇ =(variable) r₁₈ = 16.474* d₁₈ = 2.30 n_(d10) = 1.49700 V_(d10) = 81.54r₁₉ = −13.740* d₁₉ = (variable) r₂₀ = ∞ d₂₀ = 0.88 n_(d11) = 1.54771V_(d11) = 62.84 r₂₁ = ∞ d₂₁ = 0.89 r₂₂ = ∞ d₂₂ = 0.50 n_(d12) = 1.51633V_(d12) = 64.14 r₂₃ = ∞ d₂₃ = 0.60 r₂₄ = ∞ (IS) *Aspherical surface AS:Aperture stop IS: Image surface Aspherical Coefficient Fifth Surface K =0.000 A₄ = −9.52388 × 10⁻⁵ A₆ = 5.55144 × 10⁻⁶ A₈ = −3.08535 × 10⁻⁷ A₁₀= 5.48257 × 10⁻⁹ Sixth Surface K = 0.000 A₄ = 3.22716 × 10⁻⁵ A₆ =4.78631 × 10⁻⁶ A₈ = −2.53119 × 10⁻⁷ A₁₀ = 4.52425 × 10⁻⁹ 13th Surface K= 0.000 A₄ = −4.91485 × 10⁻⁵ A₆ = −7.61719 × 10⁻⁶ A₈ = 1.21791 × 10⁻⁶A₁₀ = −4.15023 × 10⁻⁸ 14th Surface K = 0.000 A₄ = 4.05960 × 10⁻⁴ A₆ =5.85350 × 10⁻⁷ A₈ = 8.56264 × 10⁻⁷ A₁₀ = −3.18996 × 10⁻⁸ 18th Surface K= 0.000 A₄ = 6.29854 × 10⁻⁴ A₆ = −3.03281 × 10⁻⁵ A₈ = 4.96221 × 10⁻⁷ A₁₀= −5.27261 × 10⁻⁸ 19th Surface K = 0.000 A₄ = 5.31709 × 10⁻⁴ A₆ =−1.74744 × 10⁻⁶ A₈ = −1.63257 × 10⁻⁶ A₁₀ = 0

TABLE 4 Zoom Data (∞) WE ST TE f (mm) 6.810 11.526 19.654 F_(NO) 3.503.95 5.00 ω(°) 30.5 18.0 10.8 d₆ 0.60 3.35 5.19 d₁₁ 5.62 2.87 1.03 d₁₂7.50 4.85 1.03 d₁₇ 2.50 5.24 9.60 d₁₉ 3.60 3.51 2.97

Example 3

TABLE 5 r₁ = −205.452 d₁ = 0.80 n_(d1) = 1.84666 V_(d1) = 23.78 r₂ =10.665 d₂ = 1.52 r₃ = ∞ d₃ = 7.40 n_(d2) = 1.80610 V_(d2) = 40.92 r₄ = ∞d₄ = 0.20 r₅ = 15.074* d₅ = 2.49 n_(d3) = 1.76802 V_(d3) = 49.24 r₆ =−14.697* d₆ = variable r₇ = 153.510 d₇ = 0.70 n_(d4) = 1.88300 V_(d4) =40.76 r₈ = 13.647 d₈ = 1.15 r₉ = −11.094 d₉ = 0.70 n_(d5) = 1.88300V_(d5) = 40.76 r₁₀ = 16.398 d₁₀ = 1.80 n_(d6) = 1.92286 V_(d6) = 20.88r₁₁ = −32.399 d₁₁ = (variable) r₁₂ = ∞ (AS) d₁₂ = (variable) r₁₃ =9.297* d₁₃ = 2.43 n_(d7) = 1.58913 V_(d7) = 61.25 r₁₄ = −24.419* d₁₄ =0.20 r₁₅ = 9.855 d₁₅ = 2.60 n_(d8) = 1.49700 V_(d8) = 81.54 r₁₆ =−150.333 d₁₆ = 0.80 r₁₇ = 19.700 d₁₇ = 1.77 n_(d9) = 1.60172 V_(d9) =60.60 r₁₈ = −32.398 d₁₈ = 0.80 n_(d10) = 1.84666 V_(d10) = 23.78 r₁₉ =4.457 d₁₉ = (variable) r₂₀ = 15.828* d₂₀ = 2.49 n_(d11) = 1.52500ν_(d11) = 55.80 r₂₁ = −15.755* d₂₁ = (variable) r₂₂ = ∞ d₂₂ = 0.88n_(d12) = 1.54771 V_(d12) = 62.84 r₂₃ = ∞ d₂₃ = 0.89 r₂₄ = ∞ d₂₄ = 0.50n_(d13) = 1.51633 V_(d13) = 64.14 r₂₅ = ∞ d₂₅ = 0.60 r₂₆ = ∞ (IS)*Aspherical surface AS: Aperture stop IS: Image surface AsphericalCoefficient Fifth Surface K = 0.000 A₄ = −1.26135 × 10⁻⁴ A₆ = 2.52905 ×10⁻⁶ A₈ = −4.00946 × 10⁻⁸ A₁₀ = −1.87589 × 10⁻⁹ Sixth Surface K = 0.000A₄ = −4.93971 × 10⁻⁶ A₆ = 3.84372 × 10⁻⁶ A₈ = −1.00573 × 10⁻⁷ A₁₀ =−6.58744 × 10⁻¹⁰ 13th Surface K = 0.000 A₄ = −2.02391 × 10⁻⁴ A₆ =−4.63863 × 10⁻⁷ A₈ = −2.67686 × 10⁻⁸ A₁₀ = −1.07522 × 10⁻⁸ 14th SurfaceK = 0.000 A₄ = 1.06475 × 10⁻⁴ A₆ = 2.61409 × 10⁻⁶ A₈ = −3.62177 × 10⁻⁷A₁₀ = 0 20th Surface K = 0.000 A₄ = 4.10682 × 10⁻⁴ A₆ = −2.65177 × 10⁻⁵A₈ = 1.17779 × 10⁻⁶ A₁₀ = −3.98281 × 10⁻⁸ 21st Surface K = 0.000 A₄ =3.52819 × 10⁻⁴ A₆ = −1.96304 × 10⁻⁵ A₈ = 7.23922 × 10⁻⁷ A₁₀ = −3.11244 ×10⁻⁸

TABLE 6 Zoom Data (∞) WE ST TE f (mm) 6.813 11.525 19.653 F_(NO) 3.574.00 5.10 ω(°) 30.6 17.9 10.9 d₆ 0.60 3.50 5.27 d₁₁ 5.56 2.66 0.90 d₁₂7.85 5.28 1.10 d₁₉ 3.00 5.69 9.96 d₂₁ 3.21 3.09 3.00

Example 4

TABLE 7 r₁ = 131.601 d₁ = 0.80 n_(d1) = 1.92286 V_(d1) = 20.88 r₂ =10.274 d₂ = 1.71 r₃ = ∞ d₃ = 7.40 n_(d2) = 1.80100 V_(d2) = 34.90 r₄ = ∞d₄ = 0.16 r₅ = 16.442* d₅ = 2.74 n_(d3) = 1.78680 V_(d3) = 44.13 r₆ =−15.303* d₆ = (variable) r₇ = −32.168 d₇ = 0.80 n_(d4) = 1.88300 V_(d4)= 40.76 r₈ = 20.848 d₈ = 0.70 r₉ = −22.286 d₉ = 0.70 n_(d5) = 1.88300V_(d5) = 40.76 r₁₀ = 11.716 d₁₀ = 1.72 n_(d6) = 1.92286 V_(d6) = 20.88r₁₁ = −119.952 d₁₁ = (variable) r₁₂ = ∞ (AS) d₁₂ = (variable) r₁₃ =8.583* d₁₃ = 3.84 n_(d7) = 1.59635 V_(d7) = 59.32 r₁₄ = −14.212* d₁₄ =0.15 r₁₅ = 8.450 d₁₅ = 3.92 n_(d8) = 1.49700 V_(d8) = 81.54 r₁₆ =−33.510 d₁₆ = 0.70 n_(d9) = 1.84666 V_(d9) = 23.78 r₁₇ = 5.517 d₁₇ =0.30 r₁₈ = 6.321 d₁₈ = 0.70 n_(d10) = 1.84666 V_(d10) = 23.78 r₁₉ =4.809 d₁₉ = (variable) r₂₀ = 17.254* d₂₀ = 2.41 n_(d11) = 1.49700V_(d11) = 81.54 r₂₁ = −12.397* d₂₁ = (variable) r₂₂ = ∞ d₂₂ = 0.88n_(d12) = 1.54771 V_(d12) = 62.84 r₂₃ = ∞ d₂₃ = 0.89 r₂₄ = ∞ d₂₄ = 0.50n_(d13) = 1.51633 V_(d13) = 64.14 r₂₅ = ∞ d₂₅ = 0.60 r₂₆ = ∞ (IS)*Aspherical surface AS: Aperture stop IS: Image surface AsphericalCoefficient Fifth Surface K = 0.000 A₄ = −8.88876 × 10⁻⁵ A₆ = −2.05062 ×10⁻⁸ A₈ = −4.57479 × 10⁻⁸ A₁₀ = −3.03644 × 10⁻¹⁰ Sixth Surface K = 0.000A₄ = 2.05704 × 10⁻⁶ A₆ = 7.72185 × 10⁻⁹ A₈ = −1.95829 × 10⁻⁸ A₁₀ =−8.08470 × 10⁻¹⁰ 13th Surface K = 0.000 A₄ = −2.57739 × 10⁻⁴ A₆ =−3.58372 × 10⁻⁶ A₈ = 2.27081 × 10⁻⁷ A₁₀ = −1.65528 × 10⁻⁸ 14th Surface K= 0.000 A₄ = 1.53919 × 10⁻⁴ A₆ = 3.18624 × 10⁻⁶ A₈ = −2.93908 × 10⁻⁷ A₁₀= −3.53209 × 10⁻⁹ 20th Surface K = 0.000 A₄ = 5.82785 × 10⁻⁴ A₆ =−2.69526 × 10⁻⁵ A₈ = 3.96147 × 10⁻⁷ A₁₀ = −5.07160 × 10⁻⁸ 21st Surface K= 0.000 A₄ = 4.65781 × 10⁻⁴ A₆ = −1.31534 × 10⁻⁶ A₈ = −1.58552 × 10⁻⁶A₁₀ = 0

TABLE 8 Zoom Data (∞) WE ST TE f (mm) 6.818 11.526 19.653 F_(NO) 3.574.00 5.10 ω(°) 30.5 18.0 10.9 d₆ 0.60 3.47 5.48 d₁₁ 5.66 2.80 0.80 d₁₂7.47 4.74 0.80 d₁₉ 2.50 5.29 9.19 d₂₁ 2.75 2.69 2.71

FIGS. 6A to 6C, 7A to 7C, 8A to 8C and 9A to 9C show aberration diagramsof Examples 1 to 4 when focused on an infinite object. In theseaberration diagrams, FIGS. 6A, 7A, 8A and 9A show a spherical aberrationSA, astigmatism AS, a distortion DT and a chromatic aberration ofmagnification (CC) in the wide-angle end. FIGS. 6B, 7B, 8B and 9B showthe above aberrations in the intermediate state. FIGS. 6C, 7C, 8C and 9Cshow the above aberrations in the telephoto end. It is to be noted thatin drawings, “FIY” denotes the image height.

Next, values of the conditions (1A) to (15A) of the above examples areshown in Table 9, and values of parameters concerning the conditions areshown in Table 10, respectively.

Example 1

TABLE 9 Condition Example 1 Example 2 Example 3 Example 4 (1A) 2.3871.991 2.080 2.213 (2A) 1.458 1.362 1.394 1.476 (3A) 0.997 0.797 0.8850.974 (4A) 0.023 0.073 −0.033 0.052 (5A) 1.808 1.764 1.755 1.777 (6A)1.725 1.690 1.691 1.692 (7A) 4.116 3.365 3.516 3.743 (8A) 2.514 2.3012.357 2.497 (9A) 0.014 0.043 −0.020 0.031 (10A) 3.117 2.981 2.966 3.006(11A) 2.667 2.468 2.495 2.599 (12A) 0.865 0.749 0.708 0.758 (13A) 1.1121.176 1.106 1.193 (14A) 5.222 3.837 3.836 3.702 (15A) 2.858 2.927 2.9562.827

TABLE 10 Parameter Example 1 Example 2 Example 3 Example 4 f_(w) 6.8986.810 6.813 6.818 f_(1G) 16.465 13.560 14.171 15.086 f_(2G) −10.056−9.274 −9.500 −10.065 f_(3G) 11.432 11.796 11.912 11.395 f_(4G) 20.89015.465 15.459 14.918 f_(L1) −12.469 −12.013 −11.955 −12.114 f_(L2)10.668 9.948 10.054 10.472 D_(2GS) 6.240 5.620 5.560 5.660 D_(S3G) 7.2107.500 7.850 7.470 R₁ 295.026 92.883 −205.452 131.601 R_(3GE) 4.449 4.7404.457 4.809 ih 4.000 4.030 4.030 4.030 m_(2GZ) 1.670 1.839 1.784 1.716m_(3GZ) 1.665 1.464 1.579 1.672

Next, there will be described a second type of zoom lens system in thepresent invention. As described above, the second type of zoom lenssystem comprises, in order from an object side: a first lens unit havinga positive refractive power; a second lens unit having a negativerefractive power; a third lens unit having a positive refractive power;a fourth lens unit having a negative refractive power; and a fifth lensunit having a positive refractive power.

The zoom lens system has five lens units in total.

During zooming from a wide-angle end toward a telephoto end, the firstlens unit is fixed, at least the second lens unit and the third lensunit move, and a space between the lens units changes. The second lensunit is positioned closer to an image-surface side in the telephoto endthan in the wide-angle end. The third lens unit is positioned closer tothe object side in the telephoto end than in the wide-angle end. Thefirst lens unit comprises a reflective optical element which reflects anoptical path.

The zoom lens system satisfies the following condition:

0.5<f _(1G) /f _(w)<3.5  (1B),

wherein f_(1G) denotes a focal length of the first lens unit, and f_(w)denotes a focal length of the zoom lens system in the wide-angle end.

The above zoom lens system includes, in order from an object, fivepositive, negative, positive, negative and positive lens units.Moreover, the second lens unit and the third lens unit are moved asdescribed above during the zooming, and the zooming function is mainlyimposed on these two lens units.

That is, when the zooming function is performed mainly by the secondlens unit, the movement amount of the second lens unit increases. Thiseasily increases the height of an off-axial ray incident upon the firstlens unit in the wide-angle end. Therefore, it becomes difficult toreduce the lens diameter of the first lens unit.

To solve the problem, in this zoom lens system, the third lens unit isalso provided with a zooming function, and the burden of the zoomingfunction imposed on the second lens unit is reduced. Accordingly, themovement amount of the second lens unit is reduced. As a result, the rayheight in the first lens unit can be reduced.

Moreover, since the negative fourth lens unit is disposed on the imageside of the positive third lens unit, the negative power of the wholelens system is divided, and an arrangement of the negative power in thezoom lens system is nearly symmetric. Therefore, even when the power ofeach lens unit is strengthened to enlarge the angle of field, to enhancethe zooming ratio and to miniaturize the lens system, the power balancedoes not easily bread down. Therefore, the lens system is advantageousin inhibiting generation of an aberration.

Moreover, the positive power of the first lens unit is set so as tosatisfy the condition (1B). In consequence, an outer diameter of thelens of the first lens unit can be reduced to reduce a bent thickness.

Below the lower limit of 0.5 of the condition (1B), the power of thefirst lens unit is strengthened, and this is advantageous inminiaturizing the first lens unit. However, in the first lens unit, alarge spherical aberration or astigmatism is generated, and it becomesdifficult to correct aberrations of the whole lens system.

On the other hand, above the upper limit of 3.5 in the condition (1B),the power of the first lens unit weakens, the movement amount of thesecond lens unit increases, and the first lens unit is easily enlargedin size. Alternatively, the positive refractive power of the third lensunit is strengthened, and it becomes difficult to reduce, with fewerlenses, aberration fluctuations generated by the movement of the thirdlens unit.

Furthermore, the fourth lens unit is effective for correcting theaberration attributable to the second lens unit. Especially when thefourth lens unit is constituted of one negative lens, theminiaturization is preferably well balanced with the aberrationcorrecting effect.

When the following constitutions are introduced in addition to the abovebasic constitution, a more satisfactory zoom lens system can beobtained.

The above zoom lens system preferably satisfies the following condition:

0.5<|f _(2G) /f _(w)|<2.0  (2B),

wherein f_(2G) is a focal length of the second lens unit.

The condition (2B) appropriately defines the power of the second lensunit. If the condition (2B) is below the lower limit of 0.5, and thepower of the second lens unit is strengthened, the movement amount ofthe second lens unit decreases, and this is advantageous in reducing thesize in the thickness direction. However, astigmatism or a distortion iseasily generated, and it becomes difficult to correct the aberrations ofthe whole lens system.

Above the upper limit of 2.0 in the condition (2B), the movement amountof the second lens unit excessively increases, and it becomes difficultto shorten the lens system in the thickness direction.

It is preferable that the above zoom lens satisfies the followingcondition:

0.6<m _(2GZ) /m _(3GZ)<1.4  (3B),

wherein m_(2GZ) denotes a ratio of the magnification of the second lensunit in the telephoto end to that in the wide-angle end when the zoomlens system is focused on an infinite object, and m_(3G) denotes a ratioof a magnification of the third lens unit in the telephoto end to thatin the wide-angle end when focused on the infinite object

The condition (3B) appropriately defines the burden of the zoomingfunction shared by the second lens unit and the third lens unit. Abovethe upper limit of 1.4 in the condition (3B), the burden of the zoomingfunction shared by the second lens unit increases, and the movementamount of the second lens unit increases. Therefore, the diameter of thefirst lens unit easily increases. Alternatively, the refractive power ofthe second lens unit increases, and the aberration fluctuations by themovement of the second lens unit are not easily reduced.

Below the lower limit of 0.6 in the condition (3B), the burden of thezooming function shared by the third lens unit increases, and themovement amount of the third lens unit easily increases. Therefore, thetotal length easily increases. Alternatively, the refractive power ofthe third lens unit increases, and the aberration fluctuations by themovement of the third lens unit are not easily reduced.

Furthermore, the above zoom lens system preferably satisfies thefollowing condition:

−0.3<f _(w) /R ₁<0.3  (4B),

wherein R₁ denotes a paraxial radius of curvature of an object-sidesurface of the lens closest to the object side in the first lens units.

The condition (4B) defines the paraxial radius of curvature of theobject-side surface of the lens closest to the object side in the firstlens unit. Below the lower limit of −0.3, a large negative distortion iseasily generated in the wide-angle end.

Above the upper limit value of 0.3 in the condition (4B), an off-axialaberration is advantageously corrected. On the other hand, the vertex ofthe lens surface easily protrudes toward the object side, and it becomesdifficult to constitute the lens system to be thin.

Moreover, in the above zoom lens system, the first lens unit ispreferably constituted of, in order from the object side, a negativemeniscus lens directing its convex surface on the object side, areflective optical element for bending the optical path, and a positivesub-unit.

When the first lens unit is provided with the reflective optical elementfor bending the optical path, there inevitably arises a tendency todeepen the entrance pupil position. Therefore, the diameter or the sizeof each optical element constituting the first lens unit increases, andthe optical path bending type system is not physically easilyestablished. Therefore, the first lens unit is constituted of, in orderfrom the object side, the negative meniscus lens directing its convexsurface on the object side, the reflective optical element for bendingthe optical path, and the positive sub-unit. According to thisconstitution, a chief ray becomes nearly parallel with the optical axisin the space required for disposing the reflective optical element, andthis can inhibit the increase of the diameter of the optical element.

To miniaturize the image taking apparatus in the height direction or thelateral direction, it is preferable that the positive sub-unit isconstituted of one positive lens.

Furthermore, the first lens unit may be constituted of, in order fromthe object side, a negative sub-unit, a reflective optical element forbending the optical path, and a positive sub-unit so that the negativesub-unit satisfies the following condition:

0.5<|f _(L1) /f _(w)|<2.5  (5B),

wherein f_(L1) denotes a focal length of the negative sub-unit of thefirst lens unit.

To constitute the entrance pupil to be shallow so that the optical pathcan physically be bent, the power of the negative sub-unit of the firstlens unit may be set to be appropriately strong as in the condition(5B).

Above the upper limit of 2.5 in the condition (5B), the entrance pupilremains to be deep. Therefore, when an angle of field is secured to acertain degree, the diameter or the size of each optical elementconstituting the first lens unit increases, and the optical path is notphysically easily bent.

Below the lower limit of 0.5 in the condition (5B), the magnification ofa lens unit or lens units, which are disposed subsequently to the firstlens unit and being constituted to move for the zooming, comes close tozero. This easily generates a problem that the movement amount increasesor the zooming ratio decreases. Moreover, it becomes difficult tocorrect an off-axial aberration such as distortion, or a chromaticaberration.

In the above zoom lens system, focusing on an object at a short distancemay be performed only by moving the fourth lens unit or the fifth lensunit toward the object side.

When the only fourth or fifth lens unit is moved to perform thefocusing, there are preferably less fluctuations of the off-axialaberration at the short distance.

In a case where the above zoom lens system is used as a photographingoptical system of the image taking apparatus, it is preferable that animage sensor is disposed on the image side of the zoom lens system, theimage sensor having a light receiving surface and converting an opticalimage formed by the zoom lens system into an electric signal.Furthermore, the following condition is preferably satisfied:

1.5<f _(w) /ih<1.9  (6B),

wherein ih denotes a maximum image height in an effective image takingregion of the light receiving surface.

The effective image taking region is a region for obtaining imageinformation for use in printing or displaying an image. The region isdisposed on the light receiving surface of the image sensor whichreceives the optical image.

The condition (6B) defines the focal length of the whole zoom lenssystem with respect to the maximum image height in the wide-angle end.Below the lower limit of 1.5 in the condition (6B), the angle of fieldin the wide-angle end unfavorably decreases.

On the other hand, above the upper limit of 1.9, the angle of fieldbecomes excessively large. To secure the bent optical path, thethickness of the zoom lens system is increased.

This condition (6B) defines the range of the focal length f_(w) in thewide-angle end in the condition (1B) or the like.

It is to be noted that the effective image taking region of the lightreceiving surface means a region for obtaining the image information foruse in printing or displaying the image. The region is disposed on thelight receiving surface of the image sensor which receives the opticalimage formed by the zoom lens system.

The above zoom lens system has a wide angle, and is advantageous inreducing the thickness or the total length.

The zoom lens system has been described above in detail, and the imagetaking apparatus has been briefly described in which the zoom lenssystem is combined with the image sensor. Next, there will be describedin more detail the image taking apparatus including the optical pathbending type zoom lens system and the image sensor.

In the present invention, a third type of image taking apparatuscomprises:

a zoom lens system; and an image sensor which is disposed on an imageside of the zoom lens system, which has a light receiving surface andwhich converts an optical image formed by the zoom lens system into anelectric signal.

The zoom lens system comprises, in order from an object side: a firstlens unit having a positive refractive power; a second lens unit havinga negative refractive power; a third lens unit having a positiverefractive power; a fourth lens unit having a negative refractive power;and a fifth lens unit having a positive refractive power. The zoom lenssystem has five lens units in total.

During zooming from a wide-angle end toward a telephoto end, the firstlens unit is fixed to an image surface on the light receiving surface,at least the second lens unit and the third lens unit move, and a spacebetween the lens units changes. The second lens unit is positionedcloser to an image-surface side in the telephoto end than in thewide-angle end. The third lens unit is positioned closer to the objectside in the telephoto end than in the wide-angle end. The first lensunit comprises a reflective optical element which reflects an opticalpath.

The apparatus satisfies the following conditions:

1.5<f _(w) /ih<1.9  (6B); and

0.85<f _(1G) /ih<6.0  (7B),

wherein f_(1G) denotes a focal length of the first lens unit, f_(w)denotes a focal length of the zoom lens system in the wide-angle end,and ih denotes a maximum image height in an effective image takingregion of the light receiving surface.

The effective image taking region is a region for obtaining imageinformation for use in printing or displaying an image. The region isdisposed on the light receiving surface of the image sensor whichreceives the optical image.

The condition (6B) defines a relation between the focal length in thewide-angle end and the maximum image height of the effective imagetaking region. Below the lower limit of 1.5 in the condition (6B), theangle of field in the wide-angle end is unfavorably reduced.

On the other hand, above the upper limit of 1.9, the angle of fieldbecomes excessively large. To secure the bent optical path, thethickness of the zoom lens system is increased.

The condition (7B) defines a relation between the focal length of thefirst lens unit and the maximum image height. The purpose of setting thecondition is similar to that of setting the condition (1B). If thecondition (7B) is below the lower limit of 0.85, and the power of thefirst lens unit is strengthened, the first lens unit is advantageouslyminiaturized. However, a spherical aberration or astigmatism is largelygenerated in the first lens unit, and it becomes difficult to correctthe aberration of the whole lens system.

On the other hand, above the upper limit of 6.0 in the condition (7B),the power of the first lens unit weakens, the movement amount of thesecond lens unit increases, and the first lens unit is easily enlargedin size. Alternatively, the positive refractive power of the third lensunit is strengthened, and it becomes difficult to reduce, with fewerlenses, aberration fluctuations generated by the movement of the thirdlens unit.

The fourth lens unit effectively corrects the aberration attributable tothe second lens unit. When the fourth lens unit is constituted of onenegative lens, both of the miniaturization and the aberration correctingeffect are preferably achieved with a good balance.

The above image taking apparatus preferably satisfies the followingcondition:

0.85<|f _(2G) /ih|<3.23  (8B),

wherein f_(2G) denotes a focal length of the second lens unit.

The condition (8B) defines a relation between the power of the secondlens unit and the maximum image height. The purpose of setting thecondition is similar to that of setting the condition (2B). If thecondition (8B) is below the lower limit of 0.85, and the power of thesecond lens unit is strengthened, the movement amount of the second lensunit decreases. This is advantageous in reducing the total length of thezoom lens system. However, astigmatism or a distortion is largelygenerated, and it becomes difficult to correct the aberration of thewhole lens system.

Above the upper limit of 3.23 in the condition (8B), the movement amountof the second lens unit becomes excessively large, and it becomesdifficult to shorten the total length.

Moreover, it is preferable that the above image taking apparatussatisfies the following condition:

0.6<m _(2GZ) /m _(3GZ)<1.4  (3B),

wherein m_(2GZ) denotes a ratio of the magnification of the second lensunit in the telephoto end to that in the wide-angle end when the zoomlens system is focused on an infinite object, and m_(3GZ) denotes aratio of the magnification of the third lens unit in the telephoto endto that in the wide-angle end when the zoom lens system is focused onthe infinite object.

The reason for the above constitution and the function and the effect ofthe constitution are as described above.

Moreover, it is preferable that the above image taking apparatussatisfies the following condition:

−0.118<ih/R ₁<0.118  (9B),

wherein R₁ denotes a paraxial radius of curvature of the object-sidesurface of a lens closest to the object side in the first lens unit.

The condition (9B) defines a relation between the paraxial radius ofcurvature of the object-side surface of the lens closest to the objectside in the first lens unit and the maximum image height. The purpose ofsetting the condition is similar to that of setting the condition (4B).Below the lower limit of −0.118, a large negative distortion is easilygenerated in the wide-angle end.

Above the upper limit value of 0.118 in the condition (9B), an off-axialaberration is advantageously corrected. However, the vertex of the lenssurface easily protrudes toward the object side, and it becomesdifficult to constitute the system to be thin.

Moreover, in the above image taking apparatus, the first lens unit ofthe zoom lens system includes, in order from the object side, a negativemeniscus lens directing its convex surface on the object side, areflective optical element for bending the optical path, and a positivesub-unit.

The reason for the above constitution and the function and the effect ofthe constitution are as described above.

Furthermore, the first lens unit may be constituted of, in order fromthe object side, a negative sub-unit, a reflective optical element forbending the optical path and a positive sub-unit so that the negativesub-unit satisfies the following condition:

0.85<|f _(L1) /ih|<4.25  (10B),

wherein f_(L1) denotes a focal length of the negative sub-unit of thefirst lens unit.

The condition (10B) defines a relation between the focal length of thenegative sub-unit constituting a front sub-unit of the first lens unitand the maximum image height. The purpose of setting the condition issimilar to that of the condition (5B), and the power of the negativesub-unit of the first lens unit may be appropriately strengthened.

Above the upper limit of 4.25 in the condition (10B), the entrance pupilremains to be deep. Therefore, when the angle of field is secured to acertain degree, the diameter or the size of each optical elementconstituting the first lens unit increases, and the optical path is notphysically easily bent.

Below the lower limit of 0.85 in the condition (10B), the magnificationof the lens unit or lens units, which are disposed subsequently to thefirst lens unit and are constituted to move for the zooming, comes closeto zero. This easily generates a problem that the movement amountincreases or the zooming ratio decreases. Moreover, it becomes difficultto correct an off-axial aberration such as the distortion, or achromatic aberration.

To miniaturize the image taking apparatus in the thickness direction,the negative sub-unit is preferably constituted of a single lens.

To miniaturize the image taking apparatus in the height direction or thelateral direction, the positive sub-unit is preferably constituted of asingle lens.

Moreover, in the above image taking apparatus, the only fourth or fifthlens unit can be moved to thereby focus on an object at a shortdistance.

The reason for the above constitution and the function and the effect ofthe constitution are as described above.

Furthermore, in the above image taking apparatus, it is preferable thatthe positive sub-unit of the first lens unit of the zoom lens systemsatisfies the following condition:

1.5<f _(L2) /ih<4.0  (11B),

wherein f_(L2) denotes a focal length of the positive sub-unit of thefirst lens unit.

The condition (11B) defines a relation between the focal length of thepositive sub-unit constituting a rear sub-unit of the first lens unitand the maximum image height. The power of the negative sub-unit of thefirst lens unit may appropriately be strengthened. However, in thiscase, an off-axial aberration such as the distortion is easilygenerated. Therefore, when an appropriately strong power is alsoimparted to the positive sub-unit disposed close to the negativesub-unit, the aberration is easily prevented from being generated. Thisis also advantageous in constituting the first lens unit to be compact.

Above the upper limit of 4.0 in the condition (11B), the power of thepositive sub-unit is reduced. This is disadvantageous in sufficientlycorrecting the off-axial aberration.

Below the lower limit of 1.5 in the condition (11B), the power of thepositive sub-unit becomes excessively strong, and it becomes difficultto correct the aberration of this lens unit.

In the above image taking apparatus, it is preferable to dispose anaperture stop between the second lens unit and the third lens unit.

This constitution is advantageous in substantially disposing the exitpupil in infinity while balancing the size of the whole lens system,that is, in constituting the whole lens system as an image-sidetelecentric optical system.

In a case where the aperture stop is disposed, the followingconstitution is especially preferable.

That is, it is preferable that the position of the aperture stop in thewide-angle end satisfies the following condition:

0.3<D _(S3G) /D _(2GS)<1.6  (12B),

wherein D_(S3G) denotes an axial length from the aperture stop to thethird lens unit in the wide-angle end, and D_(2GS) denotes an axiallength from the second lens unit to the aperture stop in the wide-angleend.

When the aperture stop is disposed close to the first lens unit and thesecond lens unit in the wide-angle end, the light beam transmittedthrough the first lens unit can be lowered. If the condition (12B) isbelow the lower limit of 0.3, and the aperture stop is separated fromthe second lens unit, it becomes difficult to constitute the first lensunit to be small.

If the condition (12B) is above the upper limit of 1.6, and the aperturestop is separated from the third lens unit, the outer diameter of thethird lens unit easily increases, and it becomes difficult to correctthe aberration in the third lens unit.

Moreover, in the above image taking apparatus, it is preferable that anaperture stop is disposed between the second lens unit and the thirdlens unit, the surface closest to the image side in the third lens unitis a concave surface, and the following conditions are satisfied:

0.3<D _(S3G) /D _(2GS)<1.6  (12B);

0.1<D _(3G4G) /D _(2GS)<1.0  (13B); and

0.5<R _(3GE) /ih<2.5  (14B),

wherein D_(S3G) denotes an axial length from the aperture stop to thethird lens unit in the wide-angle end, D_(2GS) denotes an axial lengthfrom the second lens unit to the aperture stop in the wide-angle end,D_(3G4G) denotes an axial length from the third lens unit to the fourthlens unit in the wide-angle end, and R_(3GE) denotes a paraxial radiusof curvature of the concave surface closest to the image side in thethird lens unit.

An absolute value of the curvature radius of the surface closest to theobject side in the first lens unit is reduced, or the power of the frontsub-unit having a negative refractive power is strengthened. This isadvantageous in reducing the thickness of the first lens unit. On theother hand, an off-axial aberration is easily generated in thewide-angle end.

The condition (12B) specifies the position of the aperture stop asdescribed above. Moreover, the condition (13B) defines the space betweenthe third lens unit and the fourth lens unit in the wide-angle end.

When the condition (12B) is satisfied, an incidence height of a ray uponthe first lens unit is advantageously lowered. Further, when the exitsurface of the third lens unit is constituted as a concave surface, andthe incidence height of the fourth lens unit is increased, this concavesurface and the fourth lens unit can be provided with effect ofcorrecting the off-axial aberration.

If the condition (13B) is below the lower limit of 0.1, and the spacedecreases, the incidence height of an off-axial beam upon the fourthlens unit is lowered. This is disadvantageous in correcting theoff-axial aberration in the wide-angle end. If the condition is abovethe upper limit of 1.0, and the space increases, the incidence height ofa ray excessively increases. The diameter or the total length of thelens increases. The incidence height of the off-axial beam upon thefifth lens unit also easily increases, and this is disadvantage incorrecting the aberration in this lens unit.

The condition (14B) defines a paraxial radius of curvature of theconcave surface of the third lens unit on the exit side. Below the lowerlimit of 0.5, the power of the concave surface becomes excessivelystrong, and this is disadvantageous in correcting the aberration of thethird lens unit itself. Above the upper limit of 2.5, the power of theconcave surface weakens, and the function of correcting the off-axialaberration is degraded.

Moreover, in the above image taking apparatus, it is preferable that thefourth and fifth lens units satisfy the following conditions:

4.9<|f _(4G) /ih|<20.0  (15B); and

2.0<f _(5G) /ih<5.0  (16B),

wherein f_(4G) denotes a focal length of the fourth lens unit, andf_(5G) denotes a focal length of the fifth lens unit.

The conditions (15B) and (16B) define a relation between refractivepowers of the lens units and the maximum image height in order tobalance the function of correcting the aberration by the fourth lensunit with the function of adjusting the exit pupil position of the fifthlens unit. The fourth and fifth lens units are disposed close to theimage surface. Therefore, if the conditions (15B) and (16B) are belowlower limits of 4.9 and 2.0, respectively, and the powers areexcessively strengthened, the aberration is easily generated, the lensesare increased in number, and the system is easily enlarged in size.

On the other hand, if the conditions are above upper limits of 20.0 and5.0, respectively, and the power is excessively weak, the effect ofcorrecting the off-axial aberration by the fourth lens unit is degraded.In the fifth lens unit, it becomes difficult to secure telecentricity.Alternatively, the space between the third lens unit and the fourth lensunit, or a subsequent space lengthens. This is disadvantageous inminiaturizing the apparatus.

Next, there will be described a fourth type of image taking apparatus inthe present invention.

The fourth type of image taking apparatus comprises:

a zoom lens system; and an image sensor which is disposed on an imageside of the zoom lens system, which has a light receiving surface andwhich converts an optical image formed by the zoom lens system into anelectric signal.

The zoom lens system comprises, in order from an object side: a firstlens unit having a positive refractive power; a second lens unit havinga negative refractive power; a third lens unit having a positiverefractive power; a fourth lens unit having a negative refractive power;and a fifth lens unit having a positive refractive power. The zoom lenssystem has five lens units in total.

During zooming from a wide-angle end toward a telephoto end, the firstlens unit is fixed, at least the second lens unit and the third lensunit moves, and a space between the lens units changes. The second lensunit is positioned closer to an image-surface side in the telephoto endthan in the wide-angle end. The third lens unit is positioned closer tothe object side in the telephoto end than in the wide-angle end. Thefirst lens unit comprises a reflective optical element which reflects anoptical path.

The apparatus satisfies the following conditions:

1.5<f _(w) /ih<1.9  (6B);

0.85<|f _(2G) /ih|<3.23  (8B);

1.0<f _(3G) /ih<3.7  (17B); and

0.6<m _(2GZ) /m _(3GZ)<1.4  (3B),

wherein f_(w) denotes a focal length of the zoom lens system in thewide-angle end, f_(2G) denotes a focal length of the second lens unit,f_(3G) denotes a focal length of the third lens unit, ih denotes amaximum image height in an effective image taking region of the lightreceiving surface, m_(2GZ) denotes a ratio of a magnification of thesecond lens unit in the telephoto end to that in the wide-angle end whenthe zoom lens system is focused on an infinite object, and m_(3GZ)denotes a ratio of a magnification of the third lens unit in thetelephoto end to that in the wide-angle end when the zoom lens system isfocused on the infinite object.

It is to be noted that the effective image taking region of the lightreceiving surface means a region for obtaining image information for usein printing or displaying an image. The region is disposed on the lightreceiving surface of the image sensor which receives the optical imageformed by the zoom lens system.

This image taking apparatus is advantageous in improving a performanceby devising the zoom lens system whose optical path is bent whilesecuring an angle of field.

The zoom lens system for use herein is a thin zoom lens constituted offive lens units including, in order from the object side, positive,negative, positive, negative and positive lens units. In the positivefirst lens unit, the optical path is bent by reflection. Moreover, thesecond lens unit and the third lens unit are constituted to performmovement which contributes to the zooming.

At this time, when the second lens unit largely contributes to thezooming function, the movement amount of the second lens unit increases.An incidence height of an off-axial ray upon the first lens unit easilyincreases in the wide-angle end, and it becomes difficult to reduce thelens diameter of the first lens unit.

Therefore, the third lens unit is also provided with the zoomingfunction in this zoom lens system, and the burden of the zoomingfunction imposed on the second lens unit is reduced, thereby reducingthe movement amount of the second lens unit.

Moreover, the aberration attributable to the second lens unit having thenegative refractive power is easily corrected by the negative fourthlens unit disposed on the image side of the third lens unit.

In this case, since the refractive powers of the second and third lensunits can be strengthened, the zooming ratio can be advantageouslyincreased while avoiding enlargement of the total length after theoptical path is bent.

The condition (6B) defines a relation between the focal length and themaximum image height of the effective image taking region in thewide-angle end. Below the lower limit of 1.5 in the condition (6B), theangle of field in the wide-angle end is unfavorably reduced.

On the other hand, above the upper limit of 1.9, the angle of fieldbecomes excessively large. To secure the bent optical path, thethickness of the zoom lens system is increased.

The condition (8B) defines a relation between the power of the secondlens unit and the maximum image height. If the condition (8B) is belowthe lower limit of 0.85, and the power of the second lens unit isstrengthened, the astigmatism or the distortion is largely generated,and it becomes difficult to correct the aberration of the whole lenssystem.

Above the upper limit of 3.23 in the condition (8B), the movement amountof the second lens unit becomes excessively large, and it becomesdifficult to reduce the total length.

The condition (17B) defines a relation between the power of the thirdlens unit and the maximum image height. If the condition (17B) is belowthe lower limit of 1.0, and the power of the third lens unit isstrengthened, the astigmatism or the distortion is largely generated,and it becomes difficult to correct the aberration of the whole lenssystem.

Above the upper limit of 3.7 in the condition (17B), the movement amountof the third lens unit becomes excessively large, and it becomesdifficult to reduce the total length.

The condition (3B) appropriately defines the burden of the zoomingfunction shared by the second lens unit and the third lens unit. Abovethe upper limit of 1.4 in the condition (3B), the burden of the zoomingfunction shared by the second lens unit increases, and the movementamount of the second lens unit increases. Therefore, the diameter of thefirst lens unit easily becomes large. Alternatively, the refractivepower of the second lens unit increases, and the aberration fluctuationsby the movement of the second lens unit are not easily reduced.

Below the lower limit of 0.6 in the condition (3B), the burden of thezooming function shared by the third lens unit increases, and themovement amount of the third lens unit easily increases. Therefore, thetotal length easily increases. Alternatively, the refractive power ofthe third lens unit increases, and the aberration fluctuations by themovement of the third lens unit are not easily reduced.

The fourth lens unit is advantageous in correcting the aberrationattributable to the second lens unit. When the fourth lens unit isconstituted of one negative lens, the miniaturization and the aberrationcorrecting effect are preferably achieved with a good balance.

When the fifth lens unit is constituted of one positive lens, theminiaturization and the telecentricity are preferably secured with agood balance.

Moreover, the following constitution is preferable in order tominiaturize the system and satisfactorily correct the aberration whileimposing the zooming burdens on the second and third lens units.

That is, the second lens unit is constituted of, in order from theobject side, a negative single lens having a smaller absolute value ofthe paraxial radius of curvature in an image-side surface than in anobject-side surface, and a cemented lens of a double-concave negativelens and a double-convex positive lens. The third lens unit isconstituted of, in order from the object side, a plurality of positivelenses, and one or two negative lenses. The positive lens and thenegative lens disposed adjacent to each other are cemented to constitutea cemented lens. Each of the fourth lens unit and the fifth lens unit isconstituted of two lenses or one lens.

When the second lens unit includes, in order from the object side, twonegative lenses and the double-convex positive lens, the position of theprincipal point comes close to an object. This is advantageous inreducing diameters of the first and second lens units. When a mainnegative power of the second lens unit is shared by two negative lenses,the aberration can satisfactorily be corrected. Since the cemented lensof the negative lens and the double-convex positive lens is disposed, achromatic aberration of the second lens unit itself is easily corrected.

Moreover, a main positive power of the third lens unit is shared by aplurality of positive lenses. Furthermore, since the third lens unitincludes, in order from the object side, a plurality of positive lensesand at least one negative lens, and the position of the principal pointis brought close to the object, the third lens unit can have a functionof increasing the focal length in the telephoto end.

Furthermore, when the third lens unit is provided with the cemented lensof the positive and negative lenses, the chromatic aberration is easilycorrected.

The fourth and fifth lens units are positioned closest to the imagesurface in the zoom lens system. Therefore, when the number of lensesconstituting the unit is reduced, the system is advantageouslyminiaturized. Thus, from a viewpoint of the miniaturization, it ispreferable that each of the fourth and fifth lens units is constitutedof two lenses or one lens.

The above-described constitutions can arbitrarily be satisfied,respectively. Accordingly, effects produced by the constitutions canmore preferably be obtained at the same time.

Furthermore, the image taking apparatus may be constituted to satisfy atleast one of the following constitutions.

That is, the image taking apparatus may be constituted to satisfy thefollowing condition:

0.85<f _(1G) /ih<6.0  (7B),

wherein f_(1G) denotes a focal length of the first lens unit.

Moreover, the image taking apparatus may be constituted to satisfy thefollowing condition:

−0.118<ih/R ₁<0.118  (9B),

wherein R₁ denotes a paraxial radius of curvature of an object-sidesurface of a lens closest to the object side in the first lens unit.

Furthermore, in the image taking apparatus, the first lens unit may beconstituted of, in order from the object side, a negative meniscus lensdirecting its convex surface on the object side, a reflective opticalelement for bending the optical path, and a positive sub-unit.

Furthermore, in the image taking apparatus, the first lens unit may beconstituted of, in order from the object side, a negative sub-unit, areflective optical element for bending the optical path and a positivesub-unit so that the negative sub-unit satisfies the followingcondition:

0.85<|f _(L1) /ih|<4.25  (10B),

wherein f_(L1) denotes a focal length of the negative sub-unit of thefirst lens unit.

From a viewpoint of miniaturization, it is preferable that one or bothof the positive sub-unit and the negative sub-unit is constituted of asingle lens.

Moreover, the positive sub-unit of the first lens unit may beconstituted to satisfy the following condition:

1.5<f _(L2) /ih<4.0  (11B),

wherein f_(L2) denotes a focal length of the positive sub-unit of thefirst lens unit.

Furthermore, the image taking apparatus may be constituted so as todispose an aperture stop between the second lens unit and the third lensunit.

This aperture stop is preferably disposed in the position whichsatisfies the following condition in the wide-angle end:

0.3<D _(S3G) /D _(2GS)<1.6  (12B),

wherein D_(S3G) denotes an axial length from the aperture stop to thethird lens unit in the wide-angle end, and D_(2GS) denotes an axiallength from the second lens unit to the aperture stop in the wide-angleend.

Moreover, the above image taking apparatus may be constituted so that anaperture stop is disposed between the second lens unit and the thirdlens unit, the surface closest to the image side in the third lens unitis a concave surface, and the following conditions are satisfied:

0.3<D _(S3G) /D _(2GS)<1.6  (12B);

0.1<D _(3C4G) /D _(2GS)<1.0  (13B); and

0.5<R _(3GE) /ih<2.5  (14B),

wherein D_(S3G) denotes an axial length from the aperture stop to thethird lens unit in the wide-angle end, D_(2GS) denotes an axial lengthfrom the second lens unit to the aperture stop in the wide-angle end,D_(3G4G) denotes an axial length from the third lens unit to the fourthlens unit in the wide-angle end, and R_(3GE) denotes a paraxial radiusof curvature of a concave surface closest to the image side in the thirdlens unit.

Moreover, the above image taking apparatus may be constituted so thatthe fourth and fifth lens units satisfy the following condition:

4.9<|f _(4G) /ih|<20.0  (15B); and

2.0<f _(5G) /ih<5.0  (16B),

wherein f_(4G) denotes a focal length of the fourth lens unit, andf_(5G) denotes a focal length of the fifth lens unit.

The upper and lower limit values of the above conditions (1B) to (17B)can be changed as follows.

As to the condition (1B), the lower limit value is more preferably setto 1.0, further 1.5, and the upper limit value is more preferably set to3.3, further 3.0.

As to the condition (2B), the lower limit value is more preferably setto 0.8, further 1.3, and the upper limit value is more preferably set to1.9, further 1.8.

As to the condition (3B), the lower limit value is more preferably setto 0.7, further 0.75, and the upper limit value is more preferably setto 1.2, further 1.15.

As to the condition (4B), the lower limit value is more preferably setto −0.2, further −0.15, and the upper limit value is more preferably setto 0.2, further 0.1.

As to the condition (5B), the lower limit value is more preferably setto 1.0, further 1.5, and the upper limit value is more preferably set to2.2, further 2.0.

As to the condition (6B), the lower limit value is more preferably setto 1.6, further 1.63, and the upper limit value is more preferably setto 1.8, further 1.75.

As to the condition (7B), the lower limit value is more preferably setto 1.7, further 2.55, and the upper limit value is more preferably setto 5.61, further 5.1.

As to the condition (8B), the lower limit value is more preferably setto 1.36, further 2.21, and the upper limit value is more preferably setto 3.23, further 3.06.

As to the condition (9B), the lower limit value is more preferably setto −0.118, further −0.088, and the upper limit value is more preferablyset to 0.118, further 0.059.

As to the condition (10B), the lower limit value is more preferably setto 1.7, further 2.55, and the upper limit value is more preferably setto 3.74, further 3.4.

As to the condition (11B), the lower limit value is more preferably setto 1.8, further 2.2, and the upper limit value is more preferably set to3.5, further 3.0.

As to the condition (12B), the lower limit value is more preferably setto 0.4, further 0.5, and the upper limit value is more preferably set to1.4, further 1.3.

As to the condition (13B), the lower limit value is more preferably setto 0.2, further 0.3, and the upper limit value is more preferably set to0.7, further 0.5.

As to the condition (14B), the lower limit value is more preferably setto 0.7, further 0.9, and the upper limit value is more preferably set to2.0, further 1.5.

As to the condition (15B), the lower limit value is more preferably setto 5.5, further 6.3, and the upper limit value is more preferably set to20.0, further 15.0.

As to the condition (16B), the lower limit value is more preferably setto 2.3, further 2.5, and the upper limit value is more preferably set to4.5, further 4.0.

As to the condition (17B), the lower limit value is more preferably setto 1.7, further 2.4, and the upper limit value is more preferably set to3.4, further 3.2.

It is to be noted that the above constitutions or conditions areappropriately combined to produce effects. Therefore, they are moreeffective.

The above-described optical path bending type zoom lens system and theimage taking apparatus are small in the thickness direction. Moreover,the angle of field can sufficiently be secured. The bent constitution isminiaturized while securing an optical performance and obtaining a largeangle of field. In consequence, the size of the image taking apparatuscan be reduced in the height direction or the lateral direction.

Next, there will be described numerical examples of the second type ofoptical path bending type zoom lens system.

FIGS. 10A to 12C show lens sectional views when the zoom lens system isfocused on an infinite object in Examples 5 to 7. In these drawings,FIGS. 10A, 11A and 12A are lens sectional views in a wide-angle end.FIGS. 10B, 11B and 12B are lens sectional views in an intermediatestate. FIGS. 10C, 11C and 12C are lens sectional views in a telephotoend. In these drawings: the first lens unit is denoted with G1; thesecond lens unit is denoted with G2; the aperture stop is denoted withS; the third lens unit is denoted with G3; the fourth lens unit isdenoted with G4; the fifth lens unit is denoted with G5; F denotes anoptical low pass filter having an IR cut coating surface; C denotescover glass of the electronic image sensor such as a CCD image sensor ora CMOS image sensor; and the image surface (light receiving surface) ofthe CCD image sensor, the CMOS image sensor or the like is denoted withI. Moreover, P denotes an optical path bending prism in the first lensunit G1, which is shown as a parallel flat plate developed on a straightoptical axis. It is to be noted that as shown, the surface of theoptical low pass filter F may directly be coated with an IR cut coating,or an IR cutting absorbent filter may separately be disposed.Alternatively, a transparent flat plate whose incidence surface iscoated with the IR cut coating may be used.

FIG. 13 is a diagram showing a state in which the optical path of FIG.10A is bent. The optical path bending prism P is constituted of areflective prism which bends the optical path by 90°. It is to be notedthat in Examples 5 to 7, the reflection position is in the centerbetween the incidence surface and the exit surface of the parallel flatplate P. Moreover, the reflecting direction of the optical path bendingprism P is a longitudinal direction (the vertical direction when theincident optical path is in the horizontal direction) of the imagetaking apparatus, and a short-side direction of the light receivingsurface. It is to be noted that the reflecting direction may be along-side direction of the light receiving surface.

As shown in FIGS. 10A to 10C, the zoom lens system of Example 5 isconstituted of, in order from an object side: a first lens unit G1having a positive refractive power; a second lens unit G2 having anegative refractive power; an aperture stop S; a third lens unit G3having a positive refractive power; a fourth lens unit G4 having anegative refractive power; and a fifth lens unit G5 having a positiverefractive power. When zooming is performed from a wide-angle end towarda telephoto end, the first lens unit G1 is fixed, the second lens unitG2 moves toward an image surface, the aperture stop S is substantiallyfixed, the third lens unit G3 moves toward an object, the fourth lensunit G4 moves along a locus concave toward the object while broadeningthe space between the third lens unit G3 and the fourth lens unit, thefourth lens unit is positioned closer to the object side in thetelephoto end than in the wide-angle end, and the fifth lens unit G5 isfixed.

The first lens unit G1 includes, in order from the object side, adouble-concave negative lens, an optical path bending prism P, and adouble-convex positive lens. The second lens unit G2 includes, in orderfrom the object side, a double-concave negative lens, and a cementedlens of a double-concave negative lens and a double-convex positivelens. The third lens unit G3 includes, in order from the object side, adouble-convex positive lens, and a cemented lens of a double-convexpositive lens and a double-concave negative lens. The fourth lens unitG4 includes one negative meniscus lens directing its convex surface onthe object side, and the fifth lens unit G5 includes one double-convexpositive lens.

Aspherical surfaces are used on five surfaces: opposite surfaces of thedouble-convex positive lens of the first lens unit G1; opposite surfacesof the double-convex positive lens of the third lens unit G3; and anobject-side surface of the double-convex positive lens of the fifth lensunit G5.

As shown in FIGS. 11A to 11C, the zoom lens system of Example 6 isconstituted of, in order from an object side: a first lens unit G1having a positive refractive power; a second lens unit G2 having anegative refractive power; an aperture stop S; a third lens unit G3having a positive refractive power; a fourth lens unit G4 having anegative refractive power; and a fifth lens unit G5 having a positiverefractive power. When zooming is performed from the wide-angle endtoward the telephoto end, the first lens unit G1 is fixed, the secondlens unit G2 moves toward the image surface, the aperture stop S issubstantially fixed, the third lens unit G3 moves toward the object, thefourth lens unit G4 is fixed, and the fifth lens unit G5 moves towardthe image surface.

The first lens unit G1 includes, in order from the object side, adouble-concave negative lens, an optical path bending prism P, and adouble-convex positive lens. The second lens unit G2 includes, in orderfrom the object side, a double-concave negative lens, and a cementedlens of a double-concave negative lens and a double-convex positivelens. The third lens unit G3 includes, in order from the object side, adouble-convex positive lens, and a cemented lens of a double-convexpositive lens and a double-concave negative lens. The fourth lens unitG4 includes one negative meniscus lens directing its convex surface onthe object side, and the fifth lens unit G5 includes one double-convexpositive lens.

Aspherical surfaces are used on six surfaces: opposite surfaces of thedouble-convex positive lens of the first lens unit G1; opposite surfacesof the double-convex positive lens of the third lens unit G3; andopposite surfaces of the double-convex positive lens of the fifth lensunit G5.

As shown in FIGS. 12A to 12C, the zoom lens system of Example 7 isconstituted of, in order from an object side: a first lens unit G1having a positive refractive power; a second lens unit G2 having anegative refractive power; an aperture stop S; a third lens unit G3having a positive refractive power; a fourth lens unit G4 having anegative refractive power; and a fifth lens unit G5 having a positiverefractive power. When zooming is performed from the wide-angle endtoward the telephoto end, the first lens unit G1 is fixed, the secondlens unit G2 moves toward the image surface, the aperture stop S issubstantially fixed, the third lens unit G3 moves toward the object, thefourth lens unit G4 moves along a locus concave toward the object whilebroadening the space between the third lens unit G3 and the fourth lensunit, the fourth lens unit is arranged in substantially same position inthe telephoto end as that in the wide-angle end, and the fifth lens unitG5 moves toward the image surface.

The first lens unit G1 includes, in order from the object side, anegative meniscus lens directing its convex surface on the object side,an optical path bending prism P, and a double-convex positive lens. Thesecond lens unit G2 includes, in order from the object side, apiano-concave negative lens, and a cemented lens of a double-concavenegative lens and a double-convex positive lens. The third lens unit G3includes, in order from the object side, a double-convex positive lens,and a cemented lens of a double-convex positive lens and adouble-concave negative lens. The fourth lens unit G4 includes onenegative meniscus lens directing its convex surface on the object side,and the fifth lens unit G5 includes one double-convex positive lens.

Aspherical surfaces are used on six surfaces: opposite surfaces of thedouble-convex positive lens of the first lens unit G1; opposite surfacesof the double-convex positive lens of the third lens unit G3; andopposite surfaces of the double-convex positive lens of the fifth lensunit G5.

There will be described hereinafter numeric value data of the aboveexamples. In addition to the above-described symbols: f denotes thefocal length of the whole zoom lens system; F_(NO) denotes the F number;ω denotes a half angle of field; WE denotes a wide-angle end; ST denotesan intermediate state; TE denotes a telephoto end; r₁, r₂ . . . denote aradius of curvature of each lens surface; d₁, d₂ . . . denote a spacebetween the lens surfaces; n_(d1), n_(d2) . . . denote a refractiveindex of each lens for the wavelength of the d-line; and V_(d1), V_(d2). . . denote the Abbe number of each lens. It is to be noted that anaspherical shape is represented by the following equation in which x isan optical axis whose positive direction is set to the light travelingdirection, and y has a direction crossing the optical axis at rightangles:

x=(y ² /r)/[1+{1−(K+1)(y/r)²}^(1/2) ]+A ₄ y ⁴ +A ₆ y ⁶ +A ₈ y ⁸ +A ₁₀ y¹⁰,

wherein r denotes a paraxial radius of curvature, K denotes a coniccoefficient, and A₄, A₆, A₈ and A₁₀ denote fourth-order, sixth-order,eighth-order and tenth-order aspherical coefficients, respectively.

Example 5

TABLE 11 r₁ = −52.394 d₁ = 0.84 n_(d1) = 1.81186 V_(d1) = 25.72 r₂ =10.594 d₂ = 1.37 r₃ = ∞ d₃ = 7.39 n_(d2) = 1.84666 V_(d2) = 23.78 r₄ = ∞d₄ = 0.16 r₅ = 16.429* d₅ = 2.74 n_(d3) = 1.74320 V_(d3) = 49.34 r₆ =−14.973* d₆ = variable r₇ = −52.984 d₇ = 0.84 n_(d4) = 1.88300 V_(d4) =40.76 r₈ = 32.475 d₈ = 0.63 r₉ = −17.460 d₉ = 0.84 n_(d5) = 1.88300V_(d5) = 40.76 r₁₀ = 8.037 d₁₀ = 2.14 n_(d6) = 1.84666 V_(d6) = 23.78r₁₁ = −106.964 d₁₁ = (variable) r₁₂ = ∞ (AS) d₁₂ = (variable) r₁₃ =7.537* d₁₃ = 2.20 n_(d7) = 1.74320 V_(d7) = 49.34 r₁₄ = −32.874* d₁₄ =0.21 r₁₅ = 8.885 d₁₅ = 2.44 n_(d8) = 1.69584 V_(d8) = 42.98 r₁₆ =−46.504 d₁₆ = 0.84 n_(d9) = 1.84666 V_(d9) = 23.78 r₁₇ = 4.558 d₁₇ =(variable) r₁₈ = 190.674 d₁₈ = 0.84 n_(d10) = 1.84666 V_(d10) = 23.78r₁₉ = 24.176 d₁₉ = (variable) r₂₀ = 11.544* d₂₀ = 2.20 n_(d11) = 1.49700V_(d11) = 81.54 r₂₁ = −26.422 d₂₁ = 2.33 r₂₂ = ∞ d₂₂ = 0.93 n_(d12) =1.54771 V_(d12) = 62.84 r₂₃ = ∞ d₂₃ = 0.94 r₂₄ = ∞ d₂₄ = 0.53 n_(d13) =1.51633 V_(d13) = 64.14 r₂₅ = ∞ d₂₅ = 0.60 r₂₆ = ∞ (IS) *Asphericalsurface AS: Aperture stop IS: Image surface Aspherical Coefficient FifthSurface K = 0.000 A₄ = −6.27251 × 10⁻⁵ A₆ = 4.81767 × 10⁻⁶ A₈ = −2.76647× 10⁻⁷ A₁₀ = 8.86129 × 10⁻⁹ Sixth Surface K = 0.000 A₄ = 2.76467 × 10⁻⁵A₆ = 4.35667 × 10⁻⁶ A₈ = −2.30756 × 10⁻⁷ A₁₀ = 7.75216 × 10⁻⁹ 13thSurface K = 0.000 A₄ = −1.48421 × 10⁻⁵ A₆ = 3.02417 × 10⁻⁵ A₈ = −1.65090× 10⁻⁶ A₁₀ = 1.59641 × 10⁻⁷ 14th Surface K = 0.000 A₄ = 4.53970 × 10⁻⁴A₆ = 4.70445 × 10⁻⁵ A₈ = −3.48547 × 10⁻⁶ A₁₀ = 3.17476 × 10⁻⁷ 20thSurface K = 0.000 A₄ = 4.00006 × 10⁻⁵ A₆ = −1.95270 × 10⁻⁵ A₈ = 1.78900× 10⁻⁶ A₁₀ = −6.11181 × 10⁻⁸

TABLE 12 Zoom Data (∞) WE ST TE f (mm) 6.903 11.534 19.493 F_(NO) 3.504.19 5.13 ω(°) 32.45 18.44 10.84 d₆ 0.63 4.64 8.15 d₁₁ 8.49 4.54 0.95d₁₂ 4.55 2.57 0.42 d₁₇ 3.43 5.62 7.44 d₁₉ 2.74 2.47 2.97

Example 6

TABLE 13 r₁ = −277.717 d₁ = 0.80 n_(d1) = 1.81333 V_(d1) = 24.93 r₂ =9.198 d₂ = 1.40 r₃ = ∞ d₃ = 7.42 n_(d2) = 1.84700 V_(d2) = 24.00 r₄ = ∞d₄ = 0.16 r₅ = 14.077* d₅ = 1.90 n_(d3) = 1.74320 V_(d3) = 49.34 r₆ =−17.667* d₆ = variable r₇ = −601.518 d₇ = 0.91 n_(d4) = 1.88300 V_(d4) =40.76 r₈ = 17.121 d₈ = 0.77 r₉ = −19.040 d₉ = 1.16 n_(d5) = 1.88300V_(d5) = 40.76 r₁₀ = 8.500 d₁₀ = 1.25 n_(d6) = 1.84666 V_(d6) = 23.78r₁₁ = −65.492 d₁₁ = (variable) r₁₂ = ∞ (AS) d₁₂ = (variable) r₁₃ =7.730* d₁₃ = 2.29 n_(d7) = 1.74320 V_(d7) = 49.34 r₁₄ = −28.247* d₁₄ =0.21 r₁₅ = 9.103 d₁₅ = 2.42 n_(d8) = 1.69727 V_(d8) = 44.72 r₁₆ =−48.965 d₁₆ = 0.83 n_(d9) = 1.84666 V_(d9) = 23.78 r₁₇ = 4.574 d₁₇ =(variable) r₁₈ = 30.747 d₁₈ = 0.80 n_(d10) = 1.84666 V_(d10) = 23.78 r₁₉= 12.728 d₁₉ = (variable) r₂₀ = 143.857* d₂₀ = 3.51 n_(d11) = 1.49700V_(d11) = 81.54 r₂₁ = −5.718* d₂₁ = (variable) r₂₂ = ∞ d₂₂ = 0.93n_(d12) = 1.54771 V_(d12) = 62.84 r₂₃ = ∞ d₂₃ = 0.94 r₂₄ = ∞ d₂₄ = 0.53n_(d13) = 1.51633 V_(d13) = 64.14 r₂₅ = ∞ d₂₅ = 0.10 r₂₆ = ∞ (IS)*Aspherical surface AS: Aperture stop IS: Image surface AsphericalCoefficient Fifth Surface K = 0.000 A₄ = −8.19158 × 10⁻⁵ A₆ = 3.34002 ×10⁻⁶ A₈ = −1.08892 × 10⁻⁷ A₁₀ = −5.75188 × 10⁻¹¹ Sixth Surface K = 0.000A₄ = 1.31042 × 10⁻⁶ A₆ = 4.30663 × 10⁻⁶ A₈ = −1.72904 × 10⁻⁷ A₁₀ =1.47340 × 10⁻⁹ 13th Surface K = 0.000 A₄ = 2.53436 × 10⁻⁴ A₆ = 1.89906 ×10⁻⁵ A₈ = 2.19136 × 10⁻⁷ A₁₀ = 1.07325 × 10⁻⁷ 14th Surface K = 0.000 A₄= 8.05926 × 10⁻⁴ A₆ = 4.00283 × 10⁻⁵ A₈ = −1.91638 × 10⁻⁶ A₁₀ = 3.18754× 10⁻⁷ 20th Surface K = 0.000 A₄ = −1.84316 × 10⁻⁴ A₆ = 3.22031 × 10⁻⁵A₈ = −4.64601 × 10⁻⁷ A₁₀ = −1.47014 × 10⁻⁸ 21st Surface K = 0.000 A₄ =9.95128 × 10⁻⁴ A₆ = 1.57768 × 10⁻⁵ A₈ = 1.24900 × 10⁻⁷ A₁₀ = 0

Aspherical Coefficient Fifth Surface K=0.000

A₄=−8.19158×10⁻⁵ A₆=3.34002×10⁻⁶

A₈=−1.08892×10⁻⁷ A₁₀=−5.75188×10⁻¹¹

Sixth Surface K=0.000

A₄=1.31042×10⁻⁶ A₆=4.30663×10⁻⁶

A₈=−1.72904×10⁻⁷ A₁₀=1.47340×10⁻⁹

13th Surface K=0.000

A₄=2.53436×10⁻⁴ A₆=1.89906×10⁻⁵

A₈=2.19136×10⁻⁷ A₁₀=1.07325×10⁻⁷

14th Surface K=0.000

A₄=8.05926×10⁻⁴ A₆=4.00283×10⁻⁵

A₈=−1.91638×10⁻⁶ A₁₀=3.18754×10⁻⁷

20th Surface K=0.000

A₄=−1.84316×10⁻⁴ A₆=3.22031×10⁻⁵

A₈=−4.64601×10⁻⁷ A₁₀=−1.47014×10⁻⁸

21st Surface K=0.000

A₄=9.95128×10⁻⁴ A₆=1.57768×10⁻⁵

A₈=1.24900×10⁻⁷ A₁₀=0

TABLE 14 Zoom Data (∞) WE ST TE f (mm) 6.810 11.560 19.619 F_(NO) 3.394.31 4.99 ω(°) 30.43 17.89 10.66 d₆ 0.74 4.20 8.46 d₁₁ 8.45 4.99 0.73d₁₂ 5.11 2.70 1.50 d₁₇ 3.46 5.87 7.07 d₁₉ 2.48 2.88 3.43 d₂₁ 2.64 2.231.69

Example 7

TABLE 15 r₁ = 122.393 d₁ = 0.80 n_(d1) = 1.92286 V_(d1) = 20.88 r₂ =9.887 d₂ = 1.50 r₃ = ∞ d₃ = 7.20 n_(d2) = 1.68714 V_(d2) = 50.50 r₄ = ∞d₄ = 0.15 r₅ = 16.860* d₅ = 2.30 n_(d3) = 1.77377 V_(d3) = 47.17 r₆ =−16.768* d₆ = variable r₇ = ∞ d₇ = 0.80 n_(d4) = 1.88300 V_(d4) = 40.76r₈ = 22.130 d₈ = 0.70 r₉ = −15.823 d₉ = 0.80 n_(d5) = 1.88300 V_(d5) =40.76 r₁₀ = 9.150 d₁₀ = 2.00 n_(d6) = 1.80810 V_(d6) = 22.76 r₁₁ =−42.960 d₁₁ = (variable) r₁₂ = ∞ (AS) d₁₂ = (variable) r₁₃ = 9.862* d₁₃= 2.20 n_(d7) = 1.74330 V_(d7) = 49.33 r₁₄ = −34.207* d₁₄ = 0.20 r₁₅ =6.561 d₁₅ = 4.01 n_(d8) = 1.51742 V_(d8) = 57.97 r₁₆ = −124.699 d₁₆ =0.80 n_(d9) = 1.92286 V_(d9) = 20.88 r₁₇ = 4.400 d₁₇ = (variable) r₁₈ =55.334 d₁₈ = 0.80 n_(d10) = 1.84666 V_(d10) = 23.78 r₁₉ = 23.823 d₁₉ =(variable) r₂₀ = 10.738* d₂₀ = 2.80 n_(d11) = 1.49700 V_(d11) = 81.54r₂₁ = −11.748* d₂₁ = (variable) r₂₂ = ∞ d₂₂ = 0.88 n_(d12) = 1.54771V_(d12) = 62.84 r₂₃ = ∞ d₂₃ = 0.89 r₂₄ = ∞ d₂₄ = 0.50 n_(d13) = 1.51633V_(d13) = 64.14 r₂₅ = ∞ d₂₅ = 0.60 r₂₆ = ∞ (IS) *Aspherical surface AS:Aperture stop IS: Image surface Aspherical Coefficient Fifth Surface K =0.000 A₄ = −1.93192 × 10⁻⁴ A₆ = 4.10684 × 10⁻⁶ A₈ = 1.77491 × 10⁻¹⁰ A₁₀= −1.05706 × 10⁻⁸ Sixth Surface K = 0.000 A₄ = −1.42170 × 10⁻⁴ A₆ =4.60665 × 10⁻⁶ A₈ = 7.02385 × 10⁻¹⁰ A₁₀ = −1.05899 × 10⁻⁸ 13th Surface K= 0.000 A₄ = −1.95103 × 10⁻⁷ A₆ = 2.19405 × 10⁻⁵ A₈ = 2.23919 × 10⁻⁷ A₁₀= −8.90974 × 10⁻⁹ 14th Surface K = 0.000 A₄ = 1.85441 × 10⁻⁴ A₆ =3.01532 × 10⁻⁵ A₈ = 1.73945 × 10⁻¹⁰ A₁₀ = −5.97660 × 10⁻¹¹ 20th SurfaceK = 0.000 A₄ = 8.16616 × 10⁻⁴ A₆ = −4.47035 × 10⁻⁵ A₈ = 2.00898 × 10⁻⁶A₁₀ = −1.52665 × 10⁻⁸ 21st Surface K = 0.000 A₄ = 1.52688 × 10⁻³ A₆ =−6.57459 × 10⁻⁵ A₈ = 2.10197 × 10⁻⁶ A₁₀ = 1.60992 × 10⁻¹²

Aspherical Coefficient Fifth Surface K=0.000

A₄=−1.93192×10⁻⁴ A₆=4.10684×10⁻⁶

A₈=1.77491×10⁻¹⁰ A₁₀=−1.05706×10⁻⁸

Sixth Surface K=0.000

A₄=−1.42170×10⁻⁴ A₆=4.60665×10⁻⁶

A₈=7.02385×10⁻¹⁰ A₁₀=−1.05899×10⁻⁸

13th Surface K=0.000

A₄=−1.95103×10⁻⁷ A₆=2.19405×10⁻⁵

A₈=2.23919×10⁻⁷ A₁₀=−8.90974×10⁻⁹

14th Surface K=0.000

A₄=1.85441×10⁻⁴ A₆=3.01532×10⁻⁵

A₈=1.73945×10⁻¹⁰ A₁₀=−5.97660×10⁻¹¹

20th Surface K=0.000

A₄=8.16616×10⁻⁴ A₆=−4.47035×10⁻⁵

A₈=2.00898×10⁻⁶ A₁₀=−1.52665×10⁻⁸

21st Surface K=0.000

A₄=1.52688×10⁻³ A₆=−6.57459×10⁻⁵

A₈=2.10197×10⁻⁶ A₁₀=1.60992×10⁻¹²

TABLE 16 Zoom Data (∞) WE ST TE f (mm) 6.843 11.610 19.573 F_(NO) 3.574.27 5.10 ω(°) 30.62 17.88 10.74 D₆ 0.50 3.73 6.08 D₁₁ 6.55 3.28 1.00d₁₂ 7.56 4.67 0.70 d₁₇ 2.02 4.98 8.88 d₁₉ 1.92 2.33 2.39 d₂₁ 2.21 1.771.75

FIGS. 14A to 14C, 15A to 15C and 16A to 16C show aberration diagrams ofExamples 5 to 7 when focused on an infinite object. In these aberrationdiagrams, FIGS. 14A, 15A and 16A show a spherical aberration SA, anastigmatism AS, a distortion DT and a chromatic aberration CC ofmagnification in the wide-angle end. FIGS. 14B, 15B and 16B show theabove aberrations in the intermediate state. FIGS. 14C, 15C and 16C showthe above aberrations in the telephoto end. It is to be noted that indrawings, “FIY” denotes the image height.

Next, values of the conditions (1B) to (17B) of the above examples areshown in Table 17, and values of parameters concerning the conditionsare shown in Table 18, respectively.

TABLE 17 Condition Example 5 Example 6 Example 7 (1B) 2.713 2.800 2.716(2B) 1.577 1.615 1.746 (3B) 0.883 0.755 1.105 (4B) −0.125 −0.025 0.056(5B) 1.563 1.605 1.709 (6B) 1.635 1.703 1.711 (7B) 4.436 4.766 4.646(8B) 2.579 2.750 2.987 (9B) −0.076 −0.014 0.033 (10B) 2.555 2.733 2.924(11B) 2.593 2.704 2.800 (12B) 0.536 0.605 1.154 (13B) 0.404 0.409 0.308(14B) 1.140 1.144 1.100 (15B) 7.763 6.546 12.498 (16B) 3.904 2.788 2.944(17B) 2.631 2.801 2.998

TABLE 18 Parameter Example 5 Example 6 Example 7 f_(w) 6.540 6.810 6.843f_(1G) 17.746 19.065 18.586 f_(2G) −10.316 −11.001 −11.948 f_(3G) 10.52311.205 11.992 f_(4G) −31.051 −26.185 −49.994 f_(5G) 15.614 11.152 11.775f_(L1) −10.222 −10.933 −11.695 f_(L2) 10.372 10.818 11.199 D_(2GS) 8.4908.450 6.550 D_(S3G) 4.550 5.110 7.560 D_(3G4G) 3.430 3.460 2.020 R₁−52.394 −277.717 122.393 R_(3GE) 4.558 4.574 4.400 ih 4.000 4.000 4.000m_(2GZ) 1.785 1.861 1.569 m_(3GZ) 1.576 1.404 1.735

In addition, the above optical path bending type zoom lens system can beused in an image taking apparatus in which an object image is formed byan image forming optical system and received by an image sensor such asa CCD image sensor or a CMOS image sensor to taking an object image,especially in a digital camera or a video camera, or an informationprocessing device such as a personal computer, a telephone, orespecially a cellular phone. Embodiments will be described hereinafterin which the above optical path bending type zoom lens is used in thedigital camera.

FIGS. 17 to 19 are conceptual diagrams showing a constitution in whichthe optical path bending type zoom lens is incorporated as a imageforming optical system 41 of a digital camera. FIG. 17 is a frontperspective view showing an appearance of a digital camera 40, FIG. 18is a rear view of the digital camera, and FIG. 19 is a sectional viewshowing a constitution of the digital camera 40. In this example, thedigital camera 40 includes: the image forming optical system 41 havingan image taking optical path 42; a finder optical system 43 having afinder optical path 44; a shutter release button 45; a flash lamp 46; aliquid crystal display monitor 47 and the like. When the shutter releasebutton 45 disposed in the upper portion of the camera 40 is pressed, theobject image is taken through the image forming optical system 41 inconjunction with the pressing of the button. In this embodiment, theoptical path bending type zoom optical system of Example 1 is used asshown in FIG. 19. That is, the image forming optical system is providedwith the first lens unit G1 including the optical path bending prism P,the second lens unit G2, the aperture stop S, the third lens unit G3 andthe fourth lens unit G4. The object image formed by the image formingoptical system 41 is formed on the light receiving surface of the CCDimage sensor 49 via an optical low pass filter F coated with an IR cutcoating. The object image received by the CCD image sensor 49 isdisplayed as an electronic image in the liquid crystal display monitor47 disposed in a rear surface of the camera via processing means 51.This processing means 51 is connected to recording means 52, and thephotographed electronic image can be recorded. It is to be noted thatthis recording means 52 may be disposed separately from the processingmeans 51, or may be constituted so that the image is electronicallyrecorded into and reproduced from a floppy disc, a memory card, amagneto-optical disc or the like. It is to be noted that the camera maybe constituted as a silver salt camera in which a silver salt film isdisposed instead of the CCD image sensor 49.

Furthermore, the objective optical system 53 of the finder is disposedalong the finder optical path 44. The object image formed by theobjective optical system 53 is formed on the view field frame 57 of thePorro-prism 55 which is an image erecting member. Behind the Porro-prism55, there is disposed an eyepiece optical system 59 which guides anerected image into an observer's eyeball E. It is to be noted that covermembers 50 may be disposed on an incidence side of the photographingoptical system 41 and the objective optical system 53 for the finder andan exit side of the eyepiece optical system 59, respectively.

In the digital camera 40 constituted in this manner, the image formingoptical system 41 is a small-sized and thin zoom lens which has a largeangle of field, a high zooming ratio, a satisfactorily correctedaberrations and a large aperture. A filter or the like can be disposedin the image forming optical system. Therefore, it is possible torealize miniaturization, improvement of performance and reduction ofcosts.

It is to be noted that in the example of FIG. 19, a parallel flat plateis disposed as the cover member 50, but a lens having an optical powermay be used.

The invention being thus described, it will be obvious that the same maybe varied in many ways. Such variations are not to be regarded as adeparture from the spirit and scope of the invention. Rather, the scopeof the invention shall be defined as set forth in the following claimsand their legal equivalents. All such modifications as would be obviousto one skilled in the art are intended to be included within the scopeof the following claims.

1-31. (canceled)
 32. A zoom lens system comprising, in order from anobject side: a first lens unit having a positive refractive power; asecond lens unit having a negative refractive power; a third lens unithaving a positive refractive power; a fourth lens unit having a negativerefractive power; and a fifth lens unit having a positive refractivepower, the zoom lens system having five lens units in total, duringzooming from a wide-angle end toward a telephoto end, the first lensunit being fixed, at least the second lens unit and the third lens unitbeing moved, and a space between the lens units being changed, thesecond lens unit being positioned closer to an image-surface side in thetelephoto end than in the wide-angle end, the third lens unit beingpositioned closer to the object side in the telephoto end than in thewide-angle end, the first lens unit comprising a reflective opticalelement which reflects an optical path, the zoom lens system satisfyingthe following condition:0.5<f _(1G) /f _(w)<3.5  (1B), wherein f_(1G) denotes a focal length ofthe first lens unit, and f_(w) denotes a focal length of the zoom lenssystem in the wide-angle end.
 33. The zoom lens system according toclaim 32, further satisfying the following condition:0.5<|f _(2G) /f _(w)|<2.0  (2B), wherein f_(2G) is a focal length of thesecond lens unit.
 34. The zoom lens system according to claim 32,further satisfying the following condition:0.6<m _(2GZ) /m _(3GZ)<1.4  (3B), wherein m_(2GZ) denotes a ratio of amagnification of the second lens unit in the telephoto end to that inthe wide-angle end when the zoom lens system if focused on an infiniteobject, and m_(3GZ) denotes a ratio of a magnification of the third lensunit in the telephoto end to that in the wide-angle end when the zoomlens system if focused on an infinite object.
 35. The zoom lens systemaccording to claim 32, further satisfying the following condition:−0.3<f _(w) /R ₁<0.3  (4B), wherein R₁ denotes a paraxial radius ofcurvature of an object-side surface of a lens closest to the object sidein the first lens units.
 36. The zoom lens system according to claim 32,wherein the first lens unit consists of, in order from the object side,a negative meniscus lens directing a convex surface on the object side,the reflective optical element for bending the optical path, and apositive sub-unit.
 37. The zoom lens system according to claim 32,wherein the first lens unit consists of, in order from the object side,a negative sub-unit, the reflective optical element for bending theoptical path, and a positive sub-unit, and the negative sub-unitsatisfies the following condition:0.5<|f _(L1) /f _(w)|<2.5  (5B), wherein f_(L1) denotes a focal lengthof the negative sub-unit of the first lens unit.
 38. The zoom lenssystem according to claim 32, wherein the only fourth or fifth lens unitis moved to thereby focus on an object at a short distance.
 39. An imagetaking apparatus comprising: a zoom lens system; and an image sensorwhich is disposed on an image side of the zoom lens system, which has alight receiving surface and which converts an optical image formed bythe zoom lens system into an electric signal, the zoom lens system beingthe zoom lens system according to claim 32 and satisfying the followingcondition:1.6<f _(w) /ih<1.9  (6B), wherein ih denotes a maximum image height inan effective image taking region of the light receiving surface, and theeffective image taking region is a region for obtaining imageinformation for use in printing or displaying the optical image, theregion being disposed on the image sensor which receives the opticalimage.
 40. An image taking apparatus comprises: a zoom lens system; andan image sensor which is disposed on an image side of the zoom lenssystem, which has a light receiving surface and which converts anoptical image formed by the zoom lens system into an electric signal,the zoom lens system comprising, in order from an object side: a firstlens unit having a positive refractive power; a second lens unit havinga negative refractive power; a third lens unit having a positiverefractive power; a fourth lens unit having a negative refractive power;and a fifth lens unit having a positive refractive power, the zoom lenssystem having five lens units in total, during zooming from a wide-angleend toward a telephoto end, the first lens unit being fixed to an imagesurface on the light receiving surface, at least the second lens unitand the third lens unit being moved, and a space between the lens unitsbeing changed, the second lens unit being positioned closer to animage-surface side in the telephoto end than in the wide-angle end, thethird lens unit being positioned closer to the object side in thetelephoto end than in the wide-angle end, the first lens unit comprisinga reflective optical element which reflects an optical path, theapparatus satisfying the following conditions:1.5<f _(w) /ih<1.9  (6B); and0.85<f _(1G) /ih<6.0  (7B), wherein f_(1G) denotes a focal length of thefirst lens unit, f_(w) denotes a focal length of the zoom lens system inthe wide-angle end, ih denotes a maximum image height in an effectiveimage taking region of the light receiving surface, and the effectiveimage taking region is a region for obtaining image information for usein printing or displaying the optical image, the region being disposedon the image sensor which receives the optical image.
 41. The imagetaking apparatus according to claim 40, further satisfying the followingcondition:0.85<|f _(2G) /ih|<3.23  (8B), wherein f_(2G) denotes a focal length ofthe second lens unit.
 42. The image taking apparatus according to claim40, further satisfying the following condition:0.6<m _(2GZ) /m _(3GZ)<1.4  (3B), wherein m_(2GZ) denotes a ratio of amagnification of the second lens unit in the telephoto end to that inthe wide-angle end when the zoom lens system is focused on an infiniteobject, and m_(3GZ) denotes a ratio of a magnification of the third lensunit in the telephoto end to that in the wide-angle end when the zoomlens system is focused on an infinite object.
 43. The image takingapparatus according to claim 40, further satisfying the followingcondition:−0.118<ih/R ₁<0.118  (9B), wherein R₁ denotes a paraxial radius ofcurvature of an object-side surface of a lens closest to the object sidein the first lens unit.
 44. The image taking apparatus according toclaim 40, wherein the first lens unit consists of, in order from theobject side, a negative meniscus lens directing a convex surface on theobject side, the reflective optical element which reflects the opticalpath, and positive sub-unit.
 45. The image taking apparatus according toclaim 40, wherein the first lens unit consists of, in order from theobject side, a negative sub-unit, the reflective optical element whichreflects the optical path, and a positive sub-unit, and the negativesub-unit satisfies the following condition:0.85<|f _(L1) /f _(w)|<4.25  (10B), wherein f_(L1) denotes a focallength of the negative sub-unit of the first lens unit.
 46. The imagetaking apparatus according to claim 40, wherein the only fourth or fifthlens unit is moved to thereby focus on an object at a short distance.47. The image taking apparatus according to claim 45, wherein thepositive sub-unit of the first lens unit satisfies the followingcondition:1.5<f _(L2) /ih<4.0  (11B), wherein f_(L2) denotes a focal length of thepositive sub-unit of the first lens unit.
 48. The image taking apparatusaccording to claim 40, further comprising: an aperture stop disposedbetween the second lens unit and the third lens unit.
 49. The imagetaking apparatus according to claim 48, wherein a position of theaperture stop in the wide-angle end satisfies the following condition:0.3<D _(S3G) /D _(2GS)<1.6  (12B), wherein D_(S3G) denotes an axiallength from the aperture stop to the third lens unit in the wide-angleend, and D_(2GS) denotes an axial length from the second lens unit tothe aperture stop in the wide-angle end.
 50. The image taking apparatusaccording to claim 43, further comprising: an aperture stop disposedbetween the second lens unit and the third lens unit, a surface closestto the image side in the third lens unit being a concave surface, thefollowing condition being satisfied:0.3<D _(S3G) /D _(2GS)<1.6  (12B);0.1<D _(3G4G) /D _(2GS)<1.0  (13B); and0.5<R _(3GE) /ih<2.5  (14B), wherein D_(S3G) denotes an axial lengthfrom the aperture stop to the third lens unit in the wide-angle end,D_(2GS) denotes an axial length from the second lens unit to theaperture stop in the wide-angle end, D_(3G4G) denotes an axial lengthfrom the third lens unit to the fourth lens unit in the wide-angle end,and R_(3GE) denotes a paraxial radius of curvature of the concavesurface closest to the image side in the third lens unit.
 51. The imagetaking apparatus according to claim 40, wherein the fourth lens unit andthe fifth lens unit satisfy the following condition:4.9<|f _(4G) /ih|<20.0  (15B); and2.0<f _(5G) /ih<5.0  (16B), wherein f_(4G) denotes a focal length of thefourth lens unit, and f_(5G) denotes a focal length of the fifth lensunit.
 52. An image taking apparatus comprising: a zoom lens system; andan image sensor which is disposed on an image side of the zoom lenssystem, which has a light receiving surface and which converts anoptical image formed by the zoom lens system into an electric signal,the zoom lens system comprising, in order from an object side: a firstlens unit having a positive refractive power; a second lens unit havinga negative refractive power; a third lens unit having a positiverefractive power; a fourth lens unit having a negative refractive power;and a fifth lens unit having a positive refractive power, the zoom lenssystem having five lens units in total, during zooming from a wide-angleend toward a telephoto end, the first lens unit being fixed, at leastthe second lens unit and the third lens unit being moved, and a spacebetween the lens units being changed, the second lens unit beingpositioned closer to an image-surface side in the telephoto end than inthe wide-angle end, the third lens unit being positioned closer to theobject side in the telephoto end than in the wide-angle end, the firstlens unit comprising a reflective optical element which reflects anoptical path, the apparatus satisfying the following conditions:1.5<f _(w) /ih<1.9  (6B);0.85<|f _(2G) /ih|<3.23  (8B);1.0<f _(3G) /ih<3.7  (17B); and0.6<m _(2GZ) /m _(3GZ)<1.4  (3B), wherein f_(w) denotes a focal lengthof the zoom lens system in the wide-angle end, f_(2G) denotes a focallength of the second lens unit, f_(3G) denotes a focal length of thethird lens unit, ih denotes a maximum image height in an effective imagetaking region of the light receiving surface, m_(2GZ) denotes a ratio ofa magnification of the second lens unit in the telephoto end to that inthe wide-angle end when the zoom lens system is focused on an infiniteobject, m_(3GZ) denotes a ratio of a magnification of the third lensunit in the telephoto end to that in the wide-angle end when the zoomlens system is focused on the infinite object, and the effective imagetaking region is a region for obtaining image information for use inprinting or displaying the optical image, the region being disposed onthe image sensor which receives the optical image.
 53. The image takingapparatus according to claim 52, wherein the second lens unit consistsof, in order from the object side, a negative single lens having asmaller absolute value of a paraxial radius of curvature in animage-side surface than in an object-side surface, and a cemented lensof a double-concave negative lens and a double-convex positive lens, thethird lens unit consists of, in order from the object side, a pluralityof positive lenses, and at least one negative lens, the positive lensand the negative lens disposed adjacent to each other being cemented toconstitute a cemented lens, and each of the fourth lens unit and thefifth lens unit includes not more than two lenses.
 54. The image takingapparatus according to claim 52, further satisfying the followingcondition:0.85<f _(1G) /ih<6.0  (7B), wherein f_(1G) denotes a focal length of thefirst lens unit.
 55. The image taking apparatus according to claim 52,further satisfying the following condition:−0.118<ih/R ₁<0.118  (9B), wherein R₁ denotes a paraxial radius ofcurvature of an object-side surface of a lens closest to the object sidein the first lens unit.
 56. The image taking apparatus according toclaim 52, wherein the first lens unit consists of, in order from theobject side, a negative meniscus lens directing a convex surface on theobject side, the reflective optical element for bending the opticalpath, and a positive sub-unit.
 57. The image taking apparatus accordingto claim 52, wherein the first lens unit consists of, in order from theobject side, a negative sub-unit, the reflective optical element forbending the optical path, and a positive sub-unit, and the negativesub-unit satisfies the following condition:0.85<|f _(L1) /ih|<4.25  (10B), wherein f_(L1) denotes a focal length ofthe negative sub-unit of the first lens unit.
 58. The image takingapparatus according to claim 57, wherein the positive sub-unit of thefirst lens unit satisfies the following condition:1.5<f _(L2) /ih<4.0  (11B), wherein f_(L2) denotes a focal length of thepositive sub-unit of the first lens unit.
 59. The image taking apparatusaccording to claim 52, further comprising: an aperture stop disposedbetween the second lens unit and the third lens unit.
 60. The imagetaking apparatus according to claim 59, wherein a position of theaperture stop in the wide-angle end satisfies the following condition:0.3<D _(S3G) /D _(2GS)<1.6  (12B), wherein D_(S3G) denotes an axiallength from the aperture stop to the third lens unit in the wide-angleend, and D_(2GS) denotes an axial length from the second lens unit tothe aperture stop in the wide-angle end.
 61. The image taking apparatusaccording to claim 55, further comprising: an aperture stop disposedbetween the second lens unit and the third lens unit, a surface closestto the image side in the third lens unit being a concave surface, thefollowing conditions being satisfied:0.3<D _(S3G) /D _(2GS)<1.6  (12B);0.1<D _(3G4G) /D _(2GS)<1.0  (13B); and0.5<R _(3GE) /ih<2.5  (14B), wherein D_(S3G) denotes an axial lengthfrom the aperture stop to the third lens unit in the wide-angle end,D_(2GS) denotes an axial length from the second lens unit to theaperture stop in the wide-angle end, D_(3G4G) denotes an axial lengthfrom the third lens unit to the fourth lens unit in the wide-angle end,and R_(3GE) denotes a paraxial radius of curvature of the concavesurface closest to the image side in the third lens unit.
 62. The imagetaking apparatus according to claim 52, wherein the fourth lens unit andthe fifth lens unit satisfy the following conditions:4.9<|f _(4G) /ih|<20.0  (15B); and2.0<f _(5G) /ih<5.0  (16B), wherein f_(4G) denotes a focal length of thefourth lens unit, and f_(5G) denotes a focal length of the fifth lensunit.